TWI565817B - A film forming apparatus, a sputtering cathode, and a thin film forming method - Google Patents

A film forming apparatus, a sputtering cathode, and a thin film forming method Download PDF

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TWI565817B
TWI565817B TW102137664A TW102137664A TWI565817B TW I565817 B TWI565817 B TW I565817B TW 102137664 A TW102137664 A TW 102137664A TW 102137664 A TW102137664 A TW 102137664A TW I565817 B TWI565817 B TW I565817B
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substrate
target
film forming
sputtering
source
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TW201416476A (en
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Mitsuhiro Miyauchi
Takanori Murata
Takuya Sugawara
Ichiro Shiono
Yousong Jiang
Tatsuya Hayashi
Ekishu Nagae
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Shincron Co Ltd
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    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
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    • C23C14/06Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the coating material
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    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/34Sputtering
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    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/56Apparatus specially adapted for continuous coating; Arrangements for maintaining the vacuum, e.g. vacuum locks
    • C23C14/562Apparatus specially adapted for continuous coating; Arrangements for maintaining the vacuum, e.g. vacuum locks for coating elongated substrates
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Description

薄膜形成裝置、濺鍍陰極及薄膜形成方法 Thin film forming device, sputtering cathode and film forming method

本發明係關於薄膜形成裝置、濺鍍陰極及薄膜形成方法,特別是關於能以高成膜速率於基板形成光學多層膜之薄膜形成裝置、濺鍍陰極及薄膜形成方法。 The present invention relates to a thin film forming apparatus, a sputtering cathode, and a thin film forming method, and more particularly to a thin film forming apparatus, a sputtering cathode, and a thin film forming method capable of forming an optical multilayer film on a substrate at a high deposition rate.

藉由濺鍍形成金屬化合物薄膜之方法,已知有使用高頻電源對金屬化合物靶材或金屬靶材導入反應性氣體並藉由反應性濺鍍形成薄膜之RF反應性濺鍍法或使用直流電源於金屬化合物靶材或金屬靶材導入反應性氣體並藉由反應性濺鍍形成薄膜之DC反應性濺鍍法等。 A method of forming a metal compound thin film by sputtering, and RF reactive sputtering using a high-frequency power source to introduce a reactive gas to a metal compound target or a metal target and forming a thin film by reactive sputtering or using a direct current is known. A DC reactive sputtering method in which a power source introduces a reactive gas into a metal compound target or a metal target and forms a thin film by reactive sputtering.

此處,圖8係顯示反應性氣體流量/全氣體流量比與成膜速率(薄膜之形成速度)之關係。此處,反應性氣體流量及全氣體流量係指在靶材附近之氣體流量。圖8中,反應性氣體流量比率低之區域,係與反應性氣體流量為0時大致相同之成膜速率之金屬模式A之區域。金屬模式之區域中,成膜速率對反應性氣體流量值之變動為遲鈍。 Here, FIG. 8 shows the relationship between the reactive gas flow rate/total gas flow rate ratio and the film formation rate (film formation rate). Here, the reactive gas flow rate and the total gas flow rate refer to the gas flow rate in the vicinity of the target. In Fig. 8, the region where the ratio of the reactive gas flow rate is low is the region of the metal mode A which is substantially the same film formation rate as when the flow rate of the reactive gas is zero. In the region of the metal mode, the film formation rate is slow to the change in the value of the reactive gas flow rate.

在反應性氣體流量比率較金屬模式高之區域中,成為藉由反應性氣體流量比率之上升而使成膜速率急遽地降低之遷移區域模式B,若更加增加反應性氣體流量比率,則成為成膜速率為低值且穩定、對反應性氣體流量值之變動為遲鈍之反應性模式C之區域。 In a region where the ratio of the reactive gas flow rate is higher than the metal mode, the transition region pattern B is rapidly decreased by increasing the ratio of the flow rate of the reactive gas, and if the ratio of the reactive gas flow rate is further increased, the ratio is increased. The film rate is a low value and stable region, and the change in the value of the reactive gas flow rate is a region of the retardation reactive mode C.

上述RF反應性濺鍍法或DC反應性濺鍍法,係在圖8之圖表之反應性模式C之區域進行濺鍍,當與不導入反應性氣體而形成金屬薄膜之情形對比時,為1/5~1/10程度之成膜速率。 The above RF reactive sputtering method or DC reactive sputtering method is performed by sputtering in the region of the reactive mode C of the graph of Fig. 8, and is compared with the case where a metal thin film is formed without introducing a reactive gas. Film formation rate of /5~1/10.

作為解決此種RF反應性濺鍍法或DC反應性濺鍍法中之成膜速率之降低且可形成高品質之光學多層膜之形成技術,已知有一種濺鍍方法,係於真空容器內設置自由基源,藉由以自由基使來自金屬靶材之濺鍍粒子或基板上之堆積物氧化等而形成金屬化合物(參照例如專利文獻1)。 As a technique for forming a high-quality optical multilayer film which reduces the film formation rate in such an RF reactive sputtering method or a DC reactive sputtering method, a sputtering method is known which is incorporated in a vacuum container. A radical source is provided, and a metal compound is formed by oxidizing a deposit on a sputtering target or a substrate from a metal target by a radical (see, for example, Patent Document 1).

專利文獻1所記載之濺鍍方法,係在空間上、壓力上分離真空容器內之成膜區與反應區,在成膜區進行來自金屬靶材之濺鍍後,在反應區使反應性氣體之活性種接觸於所形成之金屬薄膜,而形成金屬化合物之薄膜。 The sputtering method described in Patent Document 1 separates a film formation region and a reaction region in a vacuum vessel in a space and pressure, and performs a sputtering reaction from a metal target in a film formation region to cause a reactive gas in the reaction region. The active species contacts the formed metal film to form a thin film of the metal compound.

根據專利文獻1所記載之濺鍍方法,由於非圖8之反應性模式C而係以金屬模式A進行,因此能以高成膜速率形成光學多層膜。 According to the sputtering method described in Patent Document 1, since the reactive mode C of FIG. 8 is used in the metal mode A, the optical multilayer film can be formed at a high deposition rate.

然而,根據此專利文獻1之濺鍍方法,由於必須在空間上分離濺鍍之成膜區與進行籍由自由基之氧化、氮化之反應區且基板必須高速旋轉,因此裝置之形式限於旋轉料架型之旋轉筒式。因此,無法適用於基板對向型或直列(in-line)型之裝置。是以,能搭載之基板尺寸限定於小型,而難以對大尺寸基板成膜。 However, according to the sputtering method of Patent Document 1, since the sputtering film formation region and the reaction region by oxidation and nitridation of radicals must be spatially separated and the substrate must be rotated at a high speed, the form of the device is limited to rotation. Rotary cylinder type of rack type. Therefore, it cannot be applied to a substrate facing type or an in-line type device. Therefore, the size of the substrate that can be mounted is limited to a small size, and it is difficult to form a large-sized substrate.

[先行技術文獻] [Advanced technical literature]

專利文獻1:日本特開2001-234338(段落0067~0072,圖1) Patent Document 1: Japanese Patent Laid-Open No. 2001-234338 (paragraph 0067 to 0072, Fig. 1)

本發明有鑑於上述情事,其目的在於提供能以高成膜速率於大尺寸基板形成光學多層膜之薄膜形成裝置、濺鍍陰極及薄膜形成方法。 The present invention has been made in view of the above circumstances, and an object thereof is to provide a thin film forming apparatus, a sputtering cathode, and a thin film forming method capable of forming an optical multilayer film on a large-sized substrate at a high film formation rate.

本發明者,針對在真空槽內之靶材與活性種源之配置深入研究之結果,發現一令人驚訝之事實,即藉由使將反應性氣體激發成電漿狀態之能量源成為既定配置,即使不將靶材與活性種源在空間上及壓力上分離而設成相互在電磁性及壓力上彼此影響,仍能非以反應性模式而以金屬模式或遷移區域模式之濺鍍來形成金屬化合物薄膜,從而完成本發明。 The inventors of the present invention have found an unexpected fact that the energy source for exciting a reactive gas into a plasma state has become a predetermined configuration as a result of intensive research on the arrangement of a target and an active seed source in a vacuum chamber. Even if the target and the active seed source are not separated from each other in space and pressure, and they are mutually influenced by electromagnetic force and pressure, they can be formed by sputtering in a metal mode or a migration mode mode in a reactive mode. A thin film of a metal compound, thereby completing the present invention.

亦即,根據申請專利範圍第1項之發明,係一種薄膜形成裝置,係在 真空槽內,藉由濺鍍於基板上形成金屬化合物之薄膜,其特徵在於:於前述真空槽內具備:靶材,由金屬或具有導電性之金屬化合物構成;以及活性種源,設成與該靶材相互在電磁性及壓力上彼此影響,生成反應性氣體之活性種;前述活性種源,具備供應前述反應性氣體之氣體源、以及將能量供應至前述真空槽內以將前述反應性氣體激發成電漿狀態之能量源;前述靶材,在與前述基板之間,隔著較40mm長且為400mm以下之間隔與前述基板對向配置;前述能量源,在與前述真空槽之間具備用以將前述能量供應至前述真空槽內之介電體窗;該介電體窗,配置成相對前述基板平行或相對前述基板以90°未滿之角度往前述靶材側傾斜,藉此解決前述課題。 That is, according to the invention of claim 1 of the patent application, a film forming apparatus is attached a film for forming a metal compound by sputtering on a substrate in a vacuum chamber, comprising: a target material in the vacuum chamber; a metal or a conductive metal compound; and an active species source; The targets interact with each other electromagnetically and under pressure to form an active species of a reactive gas; the active seed source includes a gas source for supplying the reactive gas, and supplies energy to the vacuum chamber to convert the reactivity The gas is excited into an energy source in a plasma state; the target is disposed opposite to the substrate between the substrate and the substrate at a distance of 40 mm or less and 400 mm or less; the energy source is between the vacuum chamber and the vacuum chamber Providing a dielectric window for supplying the energy into the vacuum chamber; the dielectric window is disposed parallel to the substrate or inclined to the target side at an angle of 90° or less with respect to the substrate Solve the above problems.

一邊導入反應性氣體、一邊濺鍍金屬等靶材之習知反應性濺鍍,若使反應性氣體之導入量增加,則為了於靶材表面形成金屬化合物,會成為以成膜速率低之反應性模式來成膜,相較於此,本發明之薄膜形成方法,由於能非以反應性模式而以金屬模式或遷移區域模式之濺鍍來使金屬化合物成膜,因此能以高成膜速率形成光學多層膜。 Conventional reactive sputtering in which a target material such as a metal is sputtered while introducing a reactive gas, and when the amount of introduction of the reactive gas is increased, a metal compound is formed on the surface of the target to cause a reaction at a low deposition rate. In view of the film formation method, the film formation method of the present invention can form a film of a metal compound by sputtering in a metal mode or a migration mode mode in a reactive mode, thereby enabling a high film formation rate. An optical multilayer film is formed.

亦即,由於具備設成與靶材相互在電磁性及壓力上彼此影響之活性種源,因此藉由因對靶材施加電壓而產生之電漿與藉由活性種源而產生之電漿之相互作用,靶材與基板間之區域中之電漿密度即變高。其結果,靶材周邊之Ar+等濺鍍氣體活性種之量增加,濺鍍效率提升。 That is, since there is an active seed source that is designed to interact with each other electromagnetically and under pressure, the plasma generated by applying a voltage to the target and the plasma generated by the active seed source The interaction, the plasma density in the region between the target and the substrate becomes higher. As a result, the amount of the active species of the sputtering gas such as Ar + around the target increases, and the sputtering efficiency is improved.

又,由於濺鍍效率提升,因此於靶材表面形成金屬化合物前從靶材表面彈出金屬或具有導電性之金屬化合物。是以,抑制金屬化合物於靶材表面之形成,防止成膜速率之降低。 Further, since the sputtering efficiency is improved, a metal or a conductive metal compound is ejected from the surface of the target before the metal compound is formed on the surface of the target. Therefore, the formation of the metal compound on the surface of the target is suppressed, and the decrease in the film formation rate is prevented.

再者,由於以活性種源生成反應性氣體之活性種,因此即使以較少之反應性氣體量亦能得到高反應率。其結果,即使減少反應性氣體之導入量,亦能使從靶材彈出之非完全化合物之粒子及藉由此粒子堆積於基板上而形成之非完全化合物之薄膜形成物充分地反應。是以,能以金屬模式或遷移 區域模式生成金屬化合物薄膜。 Further, since the active species of the reactive gas are generated from the active seed source, a high reaction rate can be obtained even with a small amount of reactive gas. As a result, even if the introduction amount of the reactive gas is reduced, the particles of the incomplete compound ejected from the target and the film formation of the incomplete compound formed by depositing the particles on the substrate can be sufficiently reacted. Yes, can be in metal mode or migration The region mode produces a metal compound film.

又,能量源,在與真空槽之間具備用以將能量供應至真空槽內之介電體窗;介電體窗,配置成相對基板平行或相對基板以90°未滿之角度往靶材側傾斜。因此,能同時進行濺鍍金屬或具有導電性之金屬化合物靶材而使從靶材彈出之非完全化合物之粒子往基板方向飛散,及此非完全化合物之粒子堆積於基板上而形成之非完全化合物之薄膜形成物之金屬至完全化合物之轉換。其結果,不需將靶材與活性種源在空間上及壓力上分離而能設成相互在電磁性及壓力上彼此影響。 Moreover, the energy source is provided with a dielectric window for supplying energy into the vacuum chamber, and the dielectric window is arranged to be parallel to the substrate or to the target at an angle of less than 90° with respect to the substrate. Side tilt. Therefore, it is possible to simultaneously perform sputtering of a metal or a conductive metal compound target to cause particles of the incomplete compound ejected from the target to scatter in the direction of the substrate, and the particles of the incomplete compound are deposited on the substrate to form incomplete Conversion of the metal to the complete compound of the film former of the compound. As a result, it is not necessary to separate the target material from the active seed source in space and pressure, and it is possible to influence each other in electromagnetic force and pressure.

此時亦可為,前述介電體窗,配置成相對前述基板以30°以上之角度往前述靶材側傾斜,前述基板係在相對前述基板之搬送方向為垂直之方向位於與前述能量源對向之位置。 In this case, the dielectric window may be disposed to be inclined toward the target side at an angle of 30° or more with respect to the substrate, and the substrate may be positioned opposite to the energy source in a direction perpendicular to a direction in which the substrate is transported. Towards the location.

此時亦可為,具備在前述真空槽內搬送前述基板之基板搬送單元;於前述靶材之前述基板之搬送方向之上游側及下游側中之至少一方具備前述活性種源。 In this case, the substrate transfer unit that transports the substrate in the vacuum chamber may be provided, and at least one of the upstream side and the downstream side of the substrate in the transport direction of the substrate may be provided with the active seed source.

如此,由於於靶材之上游側及下游側中之至少一方具備活性種源,因此能同時進行濺鍍金屬靶材而使從靶材彈出之非完全化合物之粒子往基板方向飛散,及此非完全化合物之粒子堆積於基板上而形成之非完全化合物之薄膜形成物之金屬至完全化合物之轉換,不需將靶材與活性種源在空間上及壓力上分離而能設成相互在電磁性及壓力上彼此影響。 In this way, since at least one of the upstream side and the downstream side of the target material has an active seed source, the metal target can be simultaneously sputtered, and the particles of the incomplete compound ejected from the target can be scattered in the direction of the substrate. The conversion of the metal to the complete compound of the film formation of the incomplete compound formed by the particles of the complete compound deposited on the substrate can be set to be electromagnetic in each other without separating the target and the active seed source in space and pressure. And stress affect each other.

此時亦可為,具備在前述真空槽內搬送前述基板之基板搬送單元;於前述靶材之前述基板之搬送方向之上游側及下游側具備前述活性種源。 In this case, the substrate transfer unit that transports the substrate in the vacuum chamber may be provided, and the active seed source may be provided on the upstream side and the downstream side of the substrate in the transport direction of the substrate.

又,亦可為,控制往前述靶材導入之濺鍍氣體之流量之濺鍍氣體控制器與控制前述反應性氣體之流量之反應性氣體控制器係相互獨立設置;且具備以光學方式檢測成膜速率之檢測部;並具備控制裝置,該控制裝置係接收來自該檢測部之訊號,至少獨立控制前述濺鍍之電源及前述濺鍍氣體 控制器、以及前述活性種源之電源及前述反應性氣體控制器,來控制前述成膜速率。 Further, a sputtering gas controller that controls a flow rate of the sputtering gas introduced into the target material and a reactive gas controller that controls a flow rate of the reactive gas may be provided independently of each other; and optically detected a film rate detecting portion; and a control device for receiving a signal from the detecting portion, at least independently controlling the sputtering power source and the sputtering gas The controller, the power source of the aforementioned active seed source, and the aforementioned reactive gas controller are used to control the film formation rate.

此時,前述能量源亦可係通過前述介電體窗藉由感應耦合或表面波生成電漿之電漿源。 In this case, the energy source may also be a plasma source that generates plasma by inductive coupling or surface wave through the dielectric window.

由於如上述構成,因此能適當選擇自由基源相對基板及靶材之位置關係,而能容易地構成能以最佳條件成膜之薄膜形成裝置。 According to the above configuration, the positional relationship between the radical source and the substrate and the target can be appropriately selected, and the thin film forming apparatus capable of forming the film under optimum conditions can be easily formed.

此時,前述活性種源亦可係感應耦合型電漿(ICP)自由基源。 In this case, the active seed source may also be an inductively coupled plasma (ICP) radical source.

由於如上述構成,因此能藉由低壓力且高密度之大口徑電漿來達成高成膜速率。 With the above configuration, it is possible to achieve a high film formation rate by a large-diameter plasma having a low pressure and a high density.

此時,前述薄膜形成裝置亦可係由具備複數個成膜站之直列型濺鍍裝置構成,該成膜站包含前述靶材與設於該靶材之前述基板之搬送方向之上游側及下游側中之至少一方之前述活性種源。 In this case, the thin film forming apparatus may be configured by an in-line sputtering apparatus including a plurality of film forming stations including the target and the upstream and downstream of the transfer direction of the substrate provided in the target. The aforementioned active species source of at least one of the sides.

由於如上述構成,因此不需將以金屬模式或遷移區域模式濺鍍同時以高成膜速率形成金屬化合物薄膜之裝置構成為如習知之旋轉料架型。其結果,基板之形狀及大小不受限制,能以高成膜速率對大型基板形成金屬化合物薄膜。 Since it is constituted as described above, it is not necessary to form a device which forms a metal compound film at a high film formation rate while sputtering in a metal mode or a migration mode mode, and is configured as a conventional rotating frame type. As a result, the shape and size of the substrate are not limited, and a metal compound film can be formed on the large substrate at a high deposition rate.

此時,前述成膜站亦可具備以光學方式檢測成膜速率之檢測部;且亦可具備接收來自前述成膜速率之檢測部之訊號,以控制各該前述成膜站之個別成膜速率之控制裝置。 In this case, the film formation station may further include a detection unit that optically detects the film formation rate, or may include a signal for receiving the detection unit from the film formation rate to control the individual film formation rates of the film formation stations. Control device.

由於如上述構成,因此能藉由獨立控制濺鍍之電源及氣體流量與活性種源之電源及氣體流量等方法,進行成膜速率之反饋控制。 According to the above configuration, the film formation rate feedback control can be performed by independently controlling the power source and gas flow rate of the sputtering and the power source and gas flow rate of the active seed source.

此時亦可為,具備:濺鍍單元,在前述真空槽內濺鍍前述靶材,藉由該濺鍍從前述靶材使非完全化合物之粒子往基板飛散;以及組成轉換單元,藉由在前述真空槽內,使藉由前述活性種源生成之反應性氣體之活性種接觸於前述粒子,以轉換為金屬之完全化合物;能於前述基板上形成由 前述金屬之完全化合物構成之薄膜。 In this case, a sputtering unit may be provided in which the target material is sputtered in the vacuum chamber, and the particles of the incomplete compound are scattered from the target to the substrate by the sputtering; and the conversion unit is formed by In the vacuum chamber, an active species of a reactive gas generated by the active seed source is contacted with the particles to be converted into a complete compound of a metal; and the substrate can be formed on the substrate A film composed of a complete compound of the foregoing metal.

由於如上述構成,因此能將靶材與活性種源設成相互在電磁性及壓力上彼此影響,無需將靶材與活性種源在空間上及壓力上分離,因此能作成單純構成之薄膜形成裝置。 According to the above configuration, the target material and the active species source can be mutually influenced by electromagnetic force and pressure, and it is not necessary to separate the target material from the active seed source in space and pressure, so that a film of a simple composition can be formed. Device.

根據申請專利範圍第11項之發明,係一種濺鍍陰極,係藉由濺鍍於基板上形成金屬化合物之薄膜,其特徵在於,具備:靶材,由金屬或具有導電性之金屬化合物構成;以及活性種源,設成與該靶材相互在電磁性及壓力上彼此影響,生成反應性氣體之活性種;前述活性種源,具備供應前述反應性氣體之氣體源、以及將能量供應至前述真空槽內以將前述反應性氣體激發成電漿狀態之能量源;前述靶材,在與前述基板之間,隔著較40mm長且為400mm以下之間隔與前述基板對向配置;前述能量源,具備用以將前述能量供應至前述能量源外部之介電體窗;該介電體窗,配置成相對前述基板平行或相對前述基板以90°未滿之角度往前述靶材側傾斜,藉此解決前述課題。 According to the invention of claim 11, a sputtering cathode is a thin film formed by sputtering on a substrate to form a metal compound, characterized by comprising: a target material composed of a metal or a conductive metal compound; And an active species source, which is formed by interacting with the target electromagnetically and under pressure to generate an active species of a reactive gas; the active seed source having a gas source for supplying the reactive gas and supplying energy to the foregoing An energy source for exciting the reactive gas into a plasma state in the vacuum chamber; wherein the target material is disposed opposite to the substrate at an interval of 40 mm or longer and 400 mm or less between the substrate and the substrate; Providing a dielectric window for supplying the energy to the outside of the energy source; the dielectric window is disposed parallel to the substrate or inclined to the target side at an angle of less than 90° with respect to the substrate This solves the aforementioned problems.

一邊導入反應性氣體、一邊濺鍍金屬等靶材之習知反應性濺鍍,若使反應性氣體之導入量增加,則為了於靶材表面形成金屬化合物,會成為以成膜速率低之反應性模式來成膜,相較於此,本發明之薄膜形成方法,由於能非以反應性模式而以金屬模式或遷移區域模式之濺鍍來使金屬化合物成膜,因此能以高成膜速率形成光學多層膜。 Conventional reactive sputtering in which a target material such as a metal is sputtered while introducing a reactive gas, and when the amount of introduction of the reactive gas is increased, a metal compound is formed on the surface of the target to cause a reaction at a low deposition rate. In view of the film formation method, the film formation method of the present invention can form a film of a metal compound by sputtering in a metal mode or a migration mode mode in a reactive mode, thereby enabling a high film formation rate. An optical multilayer film is formed.

亦即,由於具備設成與靶材相互在電磁性及壓力上彼此影響之活性種源,因此藉由因對靶材施加電壓而產生之電漿與藉由活性種源而產生之電漿之相互作用,靶材與基板間之區域中之電漿密度即變高。其結果,靶材周邊之Ar+等濺鍍氣體活性種之量增加,濺鍍效率提升。 That is, since there is an active seed source that is designed to interact with each other electromagnetically and under pressure, the plasma generated by applying a voltage to the target and the plasma generated by the active seed source The interaction, the plasma density in the region between the target and the substrate becomes higher. As a result, the amount of the active species of the sputtering gas such as Ar + around the target increases, and the sputtering efficiency is improved.

又,由於濺鍍效率提升,因此於靶材表面形成金屬化合物前從靶材表面彈出金屬或具有導電性之金屬化合物。是以,抑制金屬化合物於靶材表 面之形成,防止成膜速率之降低。 Further, since the sputtering efficiency is improved, a metal or a conductive metal compound is ejected from the surface of the target before the metal compound is formed on the surface of the target. Therefore, inhibiting metal compounds on the target table The formation of the surface prevents the film formation rate from decreasing.

再者,由於以活性種源生成反應性氣體之活性種,因此即使以較少之反應性氣體量亦能得到高反應率。其結果,由於即使減少反應性氣體之導入量,亦能使彈出之非完全化合物之粒子及此粒子堆積於基板上之非完全化合物之薄膜形成物充分地反應,因此能以金屬模式或遷移區域模式生成金屬化合物薄膜。 Further, since the active species of the reactive gas are generated from the active seed source, a high reaction rate can be obtained even with a small amount of reactive gas. As a result, even if the introduction amount of the reactive gas is reduced, the particles of the incomplete compound which are ejected and the film formation of the incomplete compound in which the particles are deposited on the substrate can be sufficiently reacted, so that the metal mode or the migration region can be used. The pattern produces a metal compound film.

此時亦可為,前述靶材與前述活性種源於真空槽之同一空間內並置成產生濺蝕之前述靶材之濺鍍面與前述活性種源對向於前述基板、前述活性種源位於前述靶材之前述基板之搬送方向之上游側及下游側中之至少一方。 In this case, the target material and the active species may be disposed in the same space of the vacuum chamber, and the sputtered surface of the target which is sputtered may be located opposite to the active seed source to the substrate and the active seed source. At least one of an upstream side and a downstream side of the transfer direction of the substrate of the target.

由於如上述構成,因此藉由因對靶材施加電壓而產生之電漿與藉由活性種源而產生之電漿之相互作用,能提高靶材與基板間之區域中之電漿密度,使靶材周邊之Ar+之量增加,使濺鍍效率提升。 According to the above configuration, the plasma density generated in the region between the target and the substrate can be increased by the interaction between the plasma generated by applying a voltage to the target and the plasma generated by the active seed source. The amount of Ar + around the target increases, which increases the sputtering efficiency.

根據申請專利範圍第13項之發明,係一種薄膜形成方法,其具備:濺鍍步驟,在真空槽內,濺鍍在與前述基板之間隔著較40mm長且為400mm以下之間隔與前述基板對向配置之由金屬或具有導電性之金屬化合物構成之靶材,藉由該濺鍍從前述靶材使非完全化合物之粒子往前述基板飛散;以及組成轉換步驟,具備用以在前述真空槽內,相對前述基板為平行或相對前述基板以90°未滿之角度往前述靶材側傾斜以將能量供應至前述真空槽內的介電體窗,使藉由設成與前述靶材相互在電磁性及壓力上彼此影響之生成反應性氣體之活性種之活性種源生成之反應性氣體之活性種接觸於前述粒子,以轉換為金屬之完全化合物,藉由具備上述兩步驟,於前述基板上形成由前述金屬之完全化合物構成之薄膜,藉此解決前述課題。 According to a thirteenth aspect of the invention, there is provided a film forming method comprising: a sputtering step of sputtering a space between the substrate and the substrate at a distance of 40 mm or more and 400 mm or less in the vacuum chamber; a target made of a metal or a conductive metal compound, wherein the particles of the incomplete compound are scattered from the target to the substrate by the sputtering; and a composition conversion step is provided for use in the vacuum chamber Parallel to the substrate or inclined toward the target side at an angle of 90° with respect to the substrate to supply energy to the dielectric window in the vacuum chamber, so as to be electromagnetically arranged with the target An active species of a reactive gas generated by an active species of an active species that reacts with each other and reacts with each other in contact with each other to contact the particles to convert to a complete compound of a metal, comprising the above two steps on the substrate The above problem can be solved by forming a film composed of a complete compound of the above metal.

一邊導入反應性氣體、一邊濺鍍金屬等靶材之習知反應性濺鍍,若使反應性氣體之導入量增加,則為了於靶材表面形成金屬化合物,會成為以 成膜速率低之反應性模式來成膜,相較於此,本發明之薄膜形成方法,由於能非以反應性模式而以金屬模式或遷移區域模式之濺鍍來使金屬化合物成膜,因此能以高成膜速率形成光學多層膜。 Conventional reactive sputtering in which a target material such as a metal is sputtered while introducing a reactive gas, and when the amount of introduction of the reactive gas is increased, a metal compound is formed on the surface of the target. In the reactive mode in which the film formation rate is low, film formation is achieved. In contrast, the film formation method of the present invention can form a metal compound by sputtering in a metal mode or a migration mode mode without using a reactive mode. The optical multilayer film can be formed at a high film formation rate.

亦即,由於具備設成與靶材相互在電磁性及壓力上彼此影響之活性種源,因此藉由因對靶材施加電壓而產生之電漿與藉由活性種源而產生之電漿之相互作用,靶材與基板間之區域中之電漿密度即變高。其結果,靶材周邊之Ar+等濺鍍氣體活性種之量增加,濺鍍效率提升。 That is, since there is an active seed source that is designed to interact with each other electromagnetically and under pressure, the plasma generated by applying a voltage to the target and the plasma generated by the active seed source The interaction, the plasma density in the region between the target and the substrate becomes higher. As a result, the amount of the active species of the sputtering gas such as Ar + around the target increases, and the sputtering efficiency is improved.

又,由於濺鍍效率提升,因此於靶材表面形成金屬化合物前從靶材表面彈出金屬或具有導電性之金屬化合物。是以,抑制金屬化合物於靶材表面之形成,防止成膜速率之降低。 Further, since the sputtering efficiency is improved, a metal or a conductive metal compound is ejected from the surface of the target before the metal compound is formed on the surface of the target. Therefore, the formation of the metal compound on the surface of the target is suppressed, and the decrease in the film formation rate is prevented.

再者,由於以活性種源生成反應性氣體之活性種,因此即使以較少之反應性氣體量亦能得到高反應率。其結果,即使減少反應性氣體之導入量,亦能使彈出之非完全化合物之粒子及此粒子堆積於基板上之非完全化合物之薄膜形成物充分地反應。是以,能以金屬模式或遷移區域模式生成金屬化合物薄膜。 Further, since the active species of the reactive gas are generated from the active seed source, a high reaction rate can be obtained even with a small amount of reactive gas. As a result, even if the introduction amount of the reactive gas is reduced, the particles of the incomplete compound which are ejected and the film formation of the incomplete compound in which the particles are deposited on the substrate can be sufficiently reacted. Therefore, the metal compound film can be formed in a metal mode or a migration region mode.

又,由於使藉由設成與靶材相互在電磁性及壓力上彼此影響之活性種源生成之反應性氣體之活性種,接觸於粒子堆積於基板上之非完全化合物之薄膜形成物,藉此轉換為金屬之完全化合物,因此能將靶材與活性種源設成相互在電磁性及壓力上彼此影響,無需將活性種源與靶材在空間上及壓力上分離,因此能使用單純構成之薄膜形成裝置來成膜。 Further, by using an active species of a reactive gas generated by an active seed source which is electromagnetically and pressure-affected with each other, the thin film formation of the incomplete compound which is deposited on the substrate by the particles is borrowed. This conversion is a complete compound of metal, so that the target and the active species source can be mutually influenced by electromagnetic and pressure, and the active seed source and the target need not be spatially and pressure-separated, so that a simple composition can be used. The film forming device is used to form a film.

此時,亦可在前述組成轉換步驟後進行反覆成膜步驟,該反覆成膜步驟係將前述濺鍍步驟及前述組成轉換步驟並行反覆複數次。 At this time, the reverse film formation step may be performed after the composition conversion step, wherein the sputtering step and the composition conversion step are repeated in parallel several times.

由於如上述構成,因此能非以反應性模式而以金屬模式或遷移區域模式之濺鍍來使金屬化合物成膜,同時得到所欲膜厚之金屬化合物薄膜。 According to the above configuration, the metal compound can be formed into a film without sputtering in a metal mode or a migration region mode in a reactive mode, and a metal compound film having a desired film thickness can be obtained.

此時亦可為,在前述濺鍍步驟前進行對具備複數個成膜站之直列型薄 膜形成裝置導入前述基板之步驟,該成膜站包含前述靶材與設於該靶材之前述基板之搬送方向之上游側及下游側中之至少一方之前述活性種源;進行站內成膜步驟,該站內成膜步驟係在前述成膜站內將前述基板一邊以一定速度搬送、一邊進行前述濺鍍步驟、前述組成轉換步驟、前述反覆成膜步驟;進行將前述基板搬送至前述基板之搬送方向之前述下游側之前述成膜站之搬送步驟;進行反覆前述站內成膜步驟與前述搬送步驟之複數站成膜步驟;在位於前述基板之搬送方向之最下游之前述成膜站進行前述站內成膜步驟後,進行將前述基板排出至大氣中之步驟。 In this case, it is also possible to perform an in-line thin film having a plurality of film forming stations before the sputtering step. a step of introducing the substrate into the substrate, wherein the film formation station includes the active seed source of at least one of the target and the upstream side and the downstream side of the substrate in the transport direction of the target; and performing the in-situ film formation step The film forming step in the station performs the sputtering step, the composition conversion step, and the reverse film forming step while the substrate is transported at a constant speed in the film forming station, and transports the substrate to the substrate. a transfer step of the film formation station on the downstream side; a film formation step of repeating the in-station film formation step and the transfer step; and performing the above-described station formation at the film formation station located at the most downstream of the substrate transfer direction After the film step, a step of discharging the substrate to the atmosphere is performed.

由於如上述構成,因此能藉由適當選擇成膜站之數目來形成所欲層數之金屬化合物多層膜。 According to the above configuration, the metal compound multilayer film having a desired number of layers can be formed by appropriately selecting the number of film formation stations.

一邊導入反應性氣體、一邊濺鍍金屬等靶材之習知反應性濺鍍,若使反應性氣體之導入量增加,則為了於靶材表面形成金屬化合物,會成為以成膜速率低之反應性模式來成膜,相較於此,本發明之薄膜形成方法,由於能非以反應性模式而以金屬模式或遷移區域模式之濺鍍來使金屬化合物成膜,因此能以高成膜速率形成光學多層膜。 Conventional reactive sputtering in which a target material such as a metal is sputtered while introducing a reactive gas, and when the amount of introduction of the reactive gas is increased, a metal compound is formed on the surface of the target to cause a reaction at a low deposition rate. In view of the film formation method, the film formation method of the present invention can form a film of a metal compound by sputtering in a metal mode or a migration mode mode in a reactive mode, thereby enabling a high film formation rate. An optical multilayer film is formed.

亦即,由於具備設成與靶材相互在電磁性及壓力上彼此影響之活性種源,因此藉由因對靶材施加電壓而產生之電漿與藉由活性種源而產生之電漿之相互作用,靶材與基板間之區域中之電漿密度即變高。其結果,靶材周邊之Ar+等濺鍍氣體活性種之量增加,濺鍍效率提升。 That is, since there is an active seed source that is designed to interact with each other electromagnetically and under pressure, the plasma generated by applying a voltage to the target and the plasma generated by the active seed source The interaction, the plasma density in the region between the target and the substrate becomes higher. As a result, the amount of the active species of the sputtering gas such as Ar + around the target increases, and the sputtering efficiency is improved.

又,由於濺鍍效率提升,因此於靶材表面形成金屬化合物前從靶材表面彈出金屬或具有導電性之金屬化合物。是以,抑制金屬化合物於靶材表面之形成,防止成膜速率之降低。 Further, since the sputtering efficiency is improved, a metal or a conductive metal compound is ejected from the surface of the target before the metal compound is formed on the surface of the target. Therefore, the formation of the metal compound on the surface of the target is suppressed, and the decrease in the film formation rate is prevented.

再者,由於以活性種源生成反應性氣體之活性種,因此即使以較少之反應性氣體量亦能得到高反應率。其結果,即使減少反應性氣體之導入量,亦能使從靶材彈出之非完全化合物之粒子及藉由此粒子堆積於基板上而形 成之非完全化合物之薄膜形成物充分地反應。是以,能以金屬模式或遷移區域模式生成金屬化合物薄膜。 Further, since the active species of the reactive gas are generated from the active seed source, a high reaction rate can be obtained even with a small amount of reactive gas. As a result, even if the introduction amount of the reactive gas is reduced, the particles of the incomplete compound which are ejected from the target can be formed by depositing the particles on the substrate. The film formation of the incomplete compound is sufficiently reacted. Therefore, the metal compound film can be formed in a metal mode or a migration region mode.

A‧‧‧成膜有效區域 A‧‧‧ filming effective area

D‧‧‧距離 D‧‧‧Distance

ST,ST1~n‧‧‧成膜站 ST, ST1~n‧‧‧ filming station

1,1′‧‧‧濺鍍裝置 1,1'‧‧‧ Sputtering device

11‧‧‧裝載鎖固室 11‧‧‧Load lock chamber

12,13,32,33‧‧‧閘閥 12,13,32,33‧‧‧ gate valve

14,34‧‧‧旋轉泵 14,34‧‧‧Rotary pump

21‧‧‧成膜室 21‧‧‧ Filming room

22‧‧‧裝載用空間部 22‧‧‧Loading Space Department

23‧‧‧卸載用空間部 23‧‧‧Unloading Space Department

31‧‧‧卸載室 31‧‧‧ Unloading room

43‧‧‧基板 43‧‧‧Substrate

61‧‧‧靶材機構 61‧‧‧ Target Agency

62a,62b‧‧‧磁控濺鍍電極 62a, 62b‧‧‧Magnetron Sputtering Electrodes

63a,63b‧‧‧靶材 63a, 63b‧‧‧ targets

64‧‧‧交流電源 64‧‧‧AC power supply

65,76‧‧‧氣體瓶 65,76‧‧‧ gas bottles

66,77‧‧‧質流控制器 66,77‧‧‧Flow Controller

75,95a,95b‧‧‧配管 75, 95a, 95b‧‧‧ piping

80‧‧‧自由基源 80‧‧‧Free radical source

80A‧‧‧天線收容室 80A‧‧‧Antenna housing room

81‧‧‧盒體 81‧‧‧Box

83‧‧‧介電體板 83‧‧‧Dielectric board

84‧‧‧固定框 84‧‧‧Fixed frame

85a,85b‧‧‧天線 85a, 85b‧‧‧Antenna

86a,86b‧‧‧導線部 86a, 86b‧‧‧ lead section

87‧‧‧匹配箱 87‧‧‧match box

87a,87b‧‧‧可變電容器 87a, 87b‧‧‧variable capacitor

88‧‧‧固定具 88‧‧‧ Fixtures

88a,88b‧‧‧固定板 88a, 88b‧‧‧ fixed plate

88c,88d‧‧‧固定螺栓 88c, 88d‧‧‧ fixing bolts

89‧‧‧高頻電源 89‧‧‧High frequency power supply

95‧‧‧真空泵 95‧‧‧vacuum pump

圖1係顯示本發明一實施形態之直列型濺鍍裝置之說明圖。 Fig. 1 is an explanatory view showing an in-line sputtering apparatus according to an embodiment of the present invention.

圖2係顯示本發明一實施形態之直列型濺鍍裝置之成膜站構成之放大說明圖。 Fig. 2 is an enlarged explanatory view showing the configuration of a film formation station of the in-line sputtering apparatus according to the embodiment of the present invention.

圖3係顯示本發明一實施形態之自由基源構成之概略說明圖。 Fig. 3 is a schematic explanatory view showing the configuration of a radical source according to an embodiment of the present invention.

圖4係顯示本發明一實施形態之自由基源構成之概略說明圖。 Fig. 4 is a schematic explanatory view showing the configuration of a radical source according to an embodiment of the present invention.

圖5係顯示本發明其他實施形態之直列型濺鍍裝置之說明圖。 Fig. 5 is an explanatory view showing an in-line type sputtering apparatus according to another embodiment of the present invention.

圖6係顯示以實施例9成膜之多層AR膜在各波長之反射率、以及使第一層為物理膜厚123.9nm之Si3N4、使第二層為物理膜厚164.3nm之SiO2、使第三層為物理膜厚99.5nm之Si3N4、使第四層為物理膜厚73.2nm之SiO2之多層AR膜之膜設計在各波長之反射率對比後之圖表。 6 is a graph showing the reflectance of the multilayer AR film formed in Example 9 at each wavelength, and the Si 3 N 4 having a first layer of a physical film thickness of 123.9 nm and the second layer being a physical film thickness of 164.3 nm. 2. A graph in which the third layer is a Si 5 N 4 film having a physical film thickness of 99.5 nm, and a film of a multilayer AR film having a fourth layer of SiO 2 having a physical film thickness of 73.2 nm is designed to reflect the reflectance at each wavelength.

圖7係顯示使用本發明之一實施形態之直列型濺鍍裝置使氧氣流量增加之情形與使之減少之情形之氧分壓與靶材電壓之關連之圖表。 Fig. 7 is a graph showing the relationship between the oxygen partial pressure and the target voltage in the case where the oxygen flow rate is increased by using the in-line sputtering apparatus according to an embodiment of the present invention.

圖8係顯示一般濺鍍中之反應性氣體流量/全氣體流量比與成膜速率(薄膜之形成速度)之關係之圖表。 Fig. 8 is a graph showing the relationship between the reactive gas flow rate/total gas flow ratio in general sputtering and the film formation rate (film formation rate).

以下,參照圖說明本發明之實施形態。此外,以下說明之構件、配置等非限定本發明,當然能依照本發明之主旨進行各種改變。 Hereinafter, embodiments of the present invention will be described with reference to the drawings. Further, the members, the configurations, and the like described below are not limited to the present invention, and various changes can be made in accordance with the gist of the present invention.

本說明書中,所謂反應性氣體之活性種,係指在電漿中高速電子衝撞反應性氣體分子或原子而產生電離、解離、附著、激發等反應之結果所生成之高反應性粒子,包含反應性氣體之離子、自由基、激發種等。 In the present specification, the reactive species of a reactive gas refers to a highly reactive particle generated by a high-speed electron collision of a reactive gas molecule or an atom in a plasma to cause a reaction such as ionization, dissociation, adhesion, and excitation, and includes a reaction. Ionic ions, free radicals, excited species, etc.

所謂反應性氣體之自由基,指較反應性氣體分子更具有活性者,包含反應性氣體之分子離子、原子、內殼電子為激發狀態之自由基。 The radical of the reactive gas means a radical which is more active than the reactive gas molecule, and includes a radical of a molecular ion, an atom, and an inner shell electron of the reactive gas in an excited state.

(薄膜形成裝置) (film forming device)

作為本實施形態之薄膜形成裝置之濺鍍裝置1,係所謂裝載鎖固(load lock)式且為直列型之濺鍍裝置,由裝載鎖固室11、成膜室21、卸載室31、以及未圖示之基板搬送裝置構成。 The sputtering apparatus 1 as the film forming apparatus of the present embodiment is a load lock type in-line type sputtering apparatus, and includes a load lock chamber 11, a film formation chamber 21, an unloading chamber 31, and A substrate transfer device (not shown) is configured.

裝載鎖固室11具備用以使裝載鎖固室11開放至大氣之閘閥12、設於與成膜室21之間之閘閥13、用以將裝載鎖固室11排氣之旋轉泵14。 The load lock chamber 11 is provided with a gate valve 12 for opening the lock lock chamber 11 to the atmosphere, a gate valve 13 provided between the film forming chamber 21, and a rotary pump 14 for exhausting the load lock chamber 11.

卸載室31具備用以使卸載室31開放至大氣之閘閥32、設於與成膜室21之間之閘閥33、用以將卸載室31排氣之旋轉泵34。 The unloading chamber 31 includes a gate valve 32 for opening the unloading chamber 31 to the atmosphere, a gate valve 33 provided between the film forming chamber 21, and a rotary pump 34 for exhausting the unloading chamber 31.

未圖示之基板搬送裝置由用於直列型濺鍍裝置之公知基板搬送裝置構成,具備保持基板43之未圖示之基板保持具與未圖示之基板搬送機構。藉由基板搬送裝置,基板43從大氣中被導入裝載鎖固室11、成膜室21、卸載室31後,被往大氣中搬送。 The substrate transfer device (not shown) is configured by a known substrate transfer device for an in-line type sputtering device, and includes a substrate holder (not shown) that holds the substrate 43 and a substrate transfer mechanism (not shown). By the substrate transfer device, the substrate 43 is introduced into the load lock chamber 11, the film formation chamber 21, and the unload chamber 31 from the atmosphere, and then transported to the atmosphere.

於未圖示之基板保持具固定基板43。 The fixed substrate 43 is held by a substrate holder (not shown).

基板43由大面積之光學構件、大型之建築用窗玻璃、大型之FPD(平面面板顯示器)等所謂大尺寸基板構成。 The substrate 43 is composed of a large-sized optical member, a large-sized architectural window glass, and a large-sized FPD (flat panel display).

於未圖示之基板保持具,亦可固定一片基板43,亦可固定複數片、例如將一片基板43縱橫二等分而四分割之大小之四片基板。 In the substrate holder (not shown), a single substrate 43 may be fixed, or a plurality of sheets, for example, four substrates having a size of four divided into two in a vertical and horizontal direction, may be fixed.

於成膜室21連結複數個成膜站ST(ST1~STn)(n為正整數)而設置,成膜室21之兩端透過閘閥13,33與裝載鎖固室11、卸載室31連結。於成膜室21底面連接有排氣用之配管95b,於此配管95b連接有用以將成膜室21內排氣之真空泵95。能藉由此真空泵95與未圖示之控制器調整成膜室21內之真空度。 The film forming chamber 21 is connected to a plurality of film forming stations ST (ST1 to STn) (n is a positive integer), and both ends of the film forming chamber 21 are connected to the load lock chamber 11 and the unloading chamber 31 through the gate valves 13 and 33. A piping 95b for exhaust gas is connected to the bottom surface of the film forming chamber 21, and a vacuum pump 95 for exhausting the inside of the film forming chamber 21 is connected to the piping 95b. The degree of vacuum in the film forming chamber 21 can be adjusted by the vacuum pump 95 and a controller (not shown).

成膜室21由延伸於基板43搬送方向之中空筐體構成,於裝載鎖固室11側端部之裝載用空間部22與卸載室31側端部之卸載用空間部23之間連結有複數個成膜站ST(ST1~STn)。 The film forming chamber 21 is constituted by a hollow casing extending in the conveying direction of the substrate 43, and a plurality of connecting space portions 22 at the end portions of the loading lock chamber 11 and the unloading space portion 23 at the end portions of the unloading chamber 31 are connected to each other. Film forming stations ST (ST1~STn).

成膜站ST由兩端為了與前後之成膜站ST或裝載用空間部22、卸載用空間部23連結而形成為開口之中空筐體構成,於所有之成膜站ST1~STn內部,分別設置有靶材機構61、作為活性種源之能量源之自由基源80、以及用以從作為氣體源之氣體瓶76導入反應性氣體之配管75。 The film formation station ST is composed of a hollow casing that is formed to be open to the film formation station ST or the loading space portion 22 and the unloading space portion 23 at both ends, and is formed inside all the film formation stations ST1 to STn. A target mechanism 61, a radical source 80 as an energy source of the active seed source, and a pipe 75 for introducing a reactive gas from the gas bottle 76 as a gas source are provided.

靶材機構61如圖2所示,具備設成對向於基板43之磁控濺鍍電極62a,b、保持於磁控濺鍍電極62a,b之靶材63a,b、透過未圖示之變壓器連接於磁控濺鍍電極62a,b而能施加交變電場之交流電源64、貯存由濺鍍用之工作氣體即氬氣等惰性氣體構成之濺鍍氣體之氣體瓶65、導入貯存於氣體瓶65之濺鍍氣體之質流控制器66。 As shown in FIG. 2, the target mechanism 61 includes magnetron sputtering electrodes 62a and b which are opposed to the substrate 43, and targets 63a and b which are held by the magnetron sputtering electrodes 62a and b, and which are not shown. An AC power source 64 to which a transformer is connected to the magnetron sputtering electrodes 62a, b to apply an alternating electric field, and a gas bottle 65 for storing a sputtering gas composed of an inert gas such as argon gas, which is a working gas for sputtering, is introduced and stored. The mass flow controller 66 of the sputtering gas of the gas bottle 65.

磁控濺鍍電極62a,b設置成與保持於未圖示之基板保持具之基板43平行。 The magnetron sputtering electrodes 62a, b are provided in parallel with the substrate 43 held by the substrate holder (not shown).

靶材63a,b設置成產生濺蝕之濺鍍面與基板43平行。此處之濺蝕係指藉由濺鍍現象使靶材構成元素被彈飛而使靶材消耗之現象。 The targets 63a, b are disposed such that the sputtered sputtering surface is parallel to the substrate 43. Sputtering here refers to a phenomenon in which a target constituent element is bombarded by a sputtering phenomenon to cause a target to be consumed.

靶材63a,b由濺鍍中通常被使用之矽(Si)、鈮(Nb)、鋁(Al)、鈦(Ti)、鋯(Zr)、錫(Sn)、鉻(Cr)、鉭(Ta)、碲(Te)、鐵(Fe)、鎂(Mg)、鉿(Hf)、鎳鉻(Ni-Cr)、銦錫(In-Sn)等公知之金屬靶材或導電性之金屬化合物靶材或複合靶材構成。 The targets 63a, b are commonly used in sputtering (Si), niobium (Nb), aluminum (Al), titanium (Ti), zirconium (Zr), tin (Sn), chromium (Cr), niobium ( Known metal targets such as Ta), tellurium (Te), iron (Fe), magnesium (Mg), hafnium (Hf), nickel chromium (Ni-Cr), indium tin (In-Sn), or conductive metal compounds Target or composite target composition.

本實施形態之靶材63a,b尺寸為5×27inch,靶材63a,b與基板43之距離D為70~400mm。 The target material 63a of the present embodiment has a size of 5 × 27 inches, and the distance D between the target 63a and the substrate 43 is 70 to 400 mm.

藉由靶材63a,b之濺鍍,而於以圖2所示之成膜有效區域A使金屬化合物成膜。 The metal compound is formed into a film by the sputtering of the targets 63a, b in the film formation effective region A shown in Fig. 2.

本實施形態之交流電源64雖係由LF電源構成,但不限定於此,亦可由RF電源、雙頻RF電源等構成。 The AC power supply 64 of the present embodiment is constituted by an LF power supply. However, the present invention is not limited thereto, and may be constituted by an RF power supply, a dual-frequency RF power supply, or the like.

本實施形態中,藉由質流控制器66從氣體瓶65將氬氣等惰性氣體導至已被真空泵95調整真空度之成膜站ST,成膜站ST內之真空氣體環境氣氛被調整而進行雙磁控濺鍍。 In the present embodiment, the mass flow controller 66 guides an inert gas such as argon gas from the gas bottle 65 to the film formation station ST whose vacuum degree has been adjusted by the vacuum pump 95, and the atmosphere atmosphere of the vacuum gas in the film formation station ST is adjusted. Perform dual magnetron sputtering.

在雙磁控濺鍍中,係使用從接地電位電性絕緣之一對磁控濺鍍電極62a,b與靶材63a,b。因此,雖未圖示,但磁控濺鍍電極62a,b、靶材63a,b係透過絕緣材安裝於被接地之濺鍍裝置1本體。又,磁控濺鍍電極62a、靶材63a與濺鍍電極62b、靶材63b亦彼此電性分離。 In dual magnetron sputtering, the magnetron sputter electrodes 62a, b and the targets 63a, b are used from one of the ground potential electrical insulation. Therefore, although not shown, the magnetron sputtering electrodes 62a, b and the targets 63a, b are attached to the body of the sputtering apparatus 1 that is grounded through the insulating material. Further, the magnetron sputtering electrode 62a, the target 63a, the sputtering electrode 62b, and the target 63b are also electrically separated from each other.

在此種狀態下,將氬等工作氣體導入靶材63a,b附近並調整濺鍍環境氣氛,並從交流電源64經由未圖示之變壓器對磁控濺鍍電極62a,b施加電壓後,則恆對靶材63a,b施加交變電場。亦即,在某時點靶材63a成為陰極(負極),在該時靶材63b必定成為陽極(正極)。若在次一時點交流之方向變化,則此次靶材63b成為陰極,靶材63a成為陽極。如上述藉由一對兩個靶材63a,b交互擔負陰極與陽極之功能而形成電漿,陰極上之靶材被濺鍍而使金屬超薄膜形成於基板上。 In this state, a working gas such as argon is introduced into the vicinity of the targets 63a and b to adjust the sputtering atmosphere, and a voltage is applied from the AC power source 64 to the magnetron sputtering electrodes 62a and b via a transformer (not shown). An alternating electric field is applied to the targets 63a, b. That is, at a certain point, the target 63a becomes a cathode (negative electrode), and at this time, the target 63b is necessarily an anode (positive electrode). When the direction of the exchange at the next time point changes, the target 63b becomes the cathode and the target 63a becomes the anode. The plasma is formed by the interaction of the cathode and the anode by a pair of two targets 63a, b as described above, and the target on the cathode is sputtered to form a metal ultra-thin film on the substrate.

此時,雖亦有於陽極上附著非導電性或導電性低之不完全金屬之情形,但此陽極在藉由交變電場而被轉換為陰極時,此等不完全金屬係被濺鍍,靶材表面成為原本清淨之狀態。接著,藉由反覆此動作,即能隨時取得穩定之陽極電位狀態,防止通常與陽極電位大致相等之電漿電位之變化,穩定地從靶材63a,b往基板43使金屬粒子飛散。 At this time, although an incomplete metal having low conductivity or low conductivity is attached to the anode, when the anode is converted into a cathode by an alternating electric field, the incomplete metal is sputtered. The surface of the target becomes the original clean state. Then, by repeating this operation, the stable anode potential state can be obtained at any time, and the change in the plasma potential which is substantially equal to the anode potential can be prevented, and the metal particles can be stably scattered from the targets 63a and b to the substrate 43.

靶材63a與63b亦可僅包含相同之金屬,亦可包含異種之金屬。使用僅由相同金屬構成之靶材時,係形成包含單一金屬之薄膜,使用包含異種金屬之靶材時,係形成由合金之化合物構成之薄膜。 The targets 63a and 63b may also contain only the same metal, and may also contain a different metal. When a target composed only of the same metal is used, a film containing a single metal is formed, and when a target containing a different metal is used, a film composed of a compound of the alloy is formed.

對靶材63a,b施加之交流電壓之頻率最好為10~120KHz。 The frequency of the alternating voltage applied to the targets 63a, b is preferably 10 to 120 kHz.

自由基源80由具備高頻天線之感應耦合型電漿產生單元構成,如圖1,圖2所示,於靶材機構61之下游側設有一個,如圖3所示具有盒體81、介電體板83、固定框84、天線85a,b、固定具88、配管95a、以及真空泵95而構成。 The radical source 80 is composed of an inductively coupled plasma generating unit having a high frequency antenna. As shown in FIG. 1 and FIG. 2, one of the downstream side of the target mechanism 61 is provided, and as shown in FIG. The dielectric plate 83, the fixing frame 84, the antennas 85a, b, the fixture 88, the piping 95a, and the vacuum pump 95 are formed.

如以圖3所示,盒體81由不鏽鋼製之大致直方體之一面為開口之容器 體構成。介電體板83被固定成阻塞該開口,形成有介電體窗,較介電體窗更靠盒體81內部之側為天線收容室80A。 As shown in FIG. 3, the casing 81 is made of stainless steel and has a substantially rectangular parallelepiped as an open container. Body composition. The dielectric plate 83 is fixed to block the opening, and a dielectric window is formed. The side of the inner side of the casing 81 is the antenna housing chamber 80A.

天線收容室80A係藉由介電體板83從成膜站ST分隔而形成從成膜站ST獨立之空間。介電體板83由板狀之公知介電體構成,在本實施形態中係以石英形成。 The antenna storage chamber 80A is partitioned from the film formation station ST by the dielectric plate 83 to form a space independent of the film formation station ST. The dielectric plate 83 is made of a plate-shaped known dielectric material, and is formed of quartz in this embodiment.

固定框84由矩形框體構成。藉由以未圖示之螺栓連結固定框84與盒體81,而於固定框84與盒體81之間夾持固定有介電體板83。 The fixing frame 84 is composed of a rectangular frame. The dielectric plate 83 is sandwiched and fixed between the fixing frame 84 and the casing 81 by connecting the fixing frame 84 and the casing 81 with a bolt (not shown).

於天線收容室80A設置有天線85a,b。 Antennas 85a, b are provided in the antenna housing chamber 80A.

天線85a,b係由銅製之管狀體表面被以銀覆蓋之螺旋狀線圈電極構成,於天線收容室80A內,成螺旋之面配置成平行於盒體81之底面與介電體板83。 The antennas 85a and b are formed of a spiral coil electrode covered with silver on the surface of the tubular body made of copper. In the antenna housing chamber 80A, the spiral surface is arranged parallel to the bottom surface of the casing 81 and the dielectric plate 83.

天線85a,b並聯於高頻電源89。又,如圖4所示,天線85a,b透過導線部86a,b連接於具備可變電容器87a,b之匹配箱87,進而連接於高頻電源89。 The antennas 85a, b are connected in parallel to the high frequency power supply 89. Further, as shown in FIG. 4, the antennas 85a, b are connected to the matching box 87 including the variable capacitors 87a, b through the lead portions 86a, b, and are further connected to the high-frequency power source 89.

固定具88係以由形成有能嵌合天線85a,b之槽之板體構成之固定板88a,b與固定螺栓88c,d構成。 The fixture 88 is constituted by fixing plates 88a, b formed of a plate body in which grooves of the antennas 85a, b can be fitted, and fixing bolts 88c, d.

於固定板88a,b嵌合有天線85a,b,以固定螺栓88c,d安裝於盒體81。於盒體81在上下方向形成有複數個螺孔,固定板88a,b係使用任一螺孔安裝於盒體81。 The antennas 85a, b are fitted to the fixing plates 88a, b, and are fixed to the casing 81 by fixing bolts 88c, d. A plurality of screw holes are formed in the casing 81 in the vertical direction, and the fixing plates 88a and b are attached to the casing 81 by using any of the screw holes.

為了使天線85a,b與固定板88a,b絕緣,至少天線85a,b與於固定板88a,b之接觸面係以絕緣材形成。 In order to insulate the antennas 85a, b from the fixed plates 88a, b, at least the contact faces of the antennas 85a, b with the fixed plates 88a, b are formed of an insulating material.

於盒體81底面,如圖3所示設有排氣用之配管95a,透過閥連接有真空泵95。藉此,能操作閥使用將成膜站ST排氣之真空泵95進行天線收容室80A內之排氣。此外,圖1中,配管95a僅針對一部分之自由基源80來顯示。 As shown in Fig. 3, a piping 95a for exhausting is provided on the bottom surface of the casing 81, and a vacuum pump 95 is connected to the transmission valve. Thereby, the operable valve can be exhausted in the antenna housing chamber 80A by the vacuum pump 95 that exhausts the film forming station ST. Further, in Fig. 1, the piping 95a is displayed only for a part of the radical source 80.

本實施形態中,如圖3、圖4所示,雖係使用採用平面型螺旋狀之螺旋天線(spiral antenna)之感應耦合型電漿源,但亦可使用其他形式之感應耦合型電漿源。例如有使高頻電流流動於在玻璃管捲成螺旋狀之圓筒形螺旋天線(helical antenna)所構成之線圈者,或天線插入電漿內部之類型等。 In the present embodiment, as shown in FIGS. 3 and 4, although an inductively coupled plasma source using a planar spiral spiral antenna is used, other forms of inductively coupled plasma sources may be used. . For example, there is a type in which a high-frequency current flows through a coil formed by a helical antenna in which a glass tube is spirally wound, or a type in which an antenna is inserted into a plasma.

又,亦可使用通過介電體窗藉由感應耦合或表面波生成電漿之其他電漿源、例如電子迴旋共振(ECP)電漿源、螺旋波激發(HWP)電漿源、微波激發表面波(SWP)電漿源等。 Further, other plasma sources that generate plasma by inductive coupling or surface waves through a dielectric window, such as an electron cyclotron resonance (ECP) plasma source, a spiral wave excitation (HWP) plasma source, and a microwave excitation surface may also be used. Wave (SWP) plasma source, etc.

亦可取代感應耦合型電漿源而使用電容耦合型電漿產生源,其係於天線收容室80A內部配置平板狀之電極,對此平板狀電極施加100KHz~50MHz之高頻電力而使電漿產生。 Instead of the inductively coupled plasma source, a capacitively coupled plasma generating source may be used. The flat electrode is disposed inside the antenna housing chamber 80A, and high frequency power of 100 kHz to 50 MHz is applied to the flat electrode to make the plasma. produce.

再者,亦可使用產生感應耦合型電漿與電容耦合型電漿混存之電漿之電漿產生源。 Further, a plasma generating source which generates a plasma in which an inductively coupled plasma and a capacitively coupled plasma are mixed may be used.

於成膜站ST,於自由基源80與基板43之間如圖2所示設有配管75,透過質流控制器77連接有反應性氣體之氣體瓶76。藉此,反應性氣體能導入自由基源80與基板43之間。 In the film formation station ST, a pipe 75 is provided between the radical source 80 and the substrate 43 as shown in Fig. 2, and a gas bottle 76 of a reactive gas is connected to the mass flow controller 77. Thereby, the reactive gas can be introduced between the radical source 80 and the substrate 43.

本實施形態中,作為反應性氣體能使用氧(O2)、臭氧(O3)、一氧化二氮(N2O)等氧化性氣體、氮(N2)等氮化性氣體、甲烷(CH4)等碳化性氣體、氟(F2)、四氟化碳(CF4)等氟化性氣體等。 In the present embodiment, an oxidizing gas such as oxygen (O 2 ), ozone (O 3 ) or nitrous oxide (N 2 O), a nitriding gas such as nitrogen (N 2 ), or methane can be used as the reactive gas ( A carbonizable gas such as CH 4 ), a fluorine-containing gas such as fluorine (F 2 ) or carbon tetrafluoride (CF 4 ), or the like.

此外,本實施形態中,用以導入濺鍍氣體之質流控制器66與用以導入反應性氣體之質流控制器77係相互獨立設置,構成為能一邊監控成膜速率等、一邊獨立控制濺鍍之電源及氣體流量與活性種源之電源及氣體流量,藉此進行成膜速率之反饋控制。 Further, in the present embodiment, the mass flow controller 66 for introducing the sputtering gas and the mass flow controller 77 for introducing the reactive gas are provided independently of each other, and are configured to be independently controllable while monitoring the deposition rate and the like. The power supply and gas flow rate of the sputtering source and the power source and gas flow rate of the active seed source are used to perform feedback control of the film formation rate.

自由基源80如圖2所示,相對基板43傾斜成介電體板83之面亦即配設有介電體板83之介電體窗之面朝向基板43之中央方向。介電體板83之面與基板43之角度在0°以上且小於90°之角度之範圍內。換言之,介電體板 83與靶材63a,b平行或以0°以上且未滿90°之角度相對保持於未圖示之基板保持具之基板43傾斜設置成成膜站ST之外側接近基板43。 As shown in FIG. 2, the radical source 80 is inclined so that the surface of the dielectric plate 83, that is, the surface of the dielectric window on which the dielectric plate 83 is disposed, faces the center direction of the substrate 43. The angle between the face of the dielectric plate 83 and the substrate 43 is in the range of 0° or more and less than 90°. In other words, the dielectric plate The substrate 83 is held in parallel with the targets 63a, b or at an angle of 0° or more and less than 90°, and is inclined to the substrate 43 of the substrate holder (not shown) so that the outside of the film formation station ST is close to the substrate 43.

介電體板83之面與基板43之面之角度若為0°~60°,則成為成膜速率為最高之區域,因此較佳。 When the angle between the surface of the dielectric plate 83 and the surface of the substrate 43 is 0 to 60, the film formation rate is the highest, which is preferable.

又,各成膜站ST具備未圖示之光學式之成膜速率控制裝置,藉由以此成膜速率控制裝置控制每一成膜站ST之濺鍍條件,而能控制成膜速率以調整膜厚。 Further, each film formation station ST includes an optical film formation rate control device (not shown), and the film formation rate can be controlled by controlling the sputtering condition of each film formation station ST by the film formation rate control device. Film thickness.

未圖示之成膜速率控制裝置具備測定成膜於基板43上之薄膜膜厚之未圖示之光學式膜厚計與根據光學式膜厚計之膜厚測定結果控制質流控制器66、77以控制氣體流量之未圖示控制裝置。 The film formation rate control device (not shown) includes an optical film thickness meter (not shown) that measures the thickness of the film formed on the substrate 43 and the film thickness measurement result according to the optical film thickness meter. 77 is a control device not shown to control the flow of gas.

光學式膜厚計雖係使用從投光器射出光並測定透射過光學薄膜之光線之透射式光學式膜厚計,但亦可使用反射式之光學式膜厚計,其係利用藉由在光學薄膜表面上反射之光線與在基板與光學膜之界面反射之光線因路徑差異產生相位差而干涉之現象來測定膜厚。 The optical film thickness meter uses a transmissive optical film thickness meter that emits light from a light projector and measures light transmitted through the optical film. However, a reflective optical film thickness meter may be used, which is used in an optical film. The film thickness is measured by a phenomenon in which the light reflected on the surface and the light reflected at the interface between the substrate and the optical film interfere with each other due to a phase difference.

在進行濺鍍之期間中,於各成膜站ST藉由未圖示之光學式膜厚計對基板43上進行成膜中之薄膜膜厚之監控,當光學式膜厚計檢測出成膜速度降低時,即增加來自交流電源64及高頻電源89之電流量,進行使已下降之成膜速度恢復成原本速度之控制。 During the sputtering process, the film thickness of the film formed on the substrate 43 is monitored by an optical film thickness meter (not shown) in each film formation station ST, and film formation is detected by the optical film thickness meter. When the speed is lowered, the amount of current from the AC power source 64 and the high-frequency power source 89 is increased, and control is performed to restore the lowered film forming speed to the original speed.

本實施形態之自由基源80係在將天線收容室80A內保持於較成膜站ST內低之壓力之狀態下,將氣體瓶76內之反應性氣體經由質流控制器77導入成膜站ST。從高頻電源89對天線85a,b施加13.56MHz之電壓,使高頻電流流動。藉此,抑制於天線收容室80A內產生電漿,天線85a,b從高頻電源89接收電力之供應,使成膜站ST內部產生感應電場,使反應性氣體之電漿產生。 In the state in which the radical source 80 of the present embodiment is held in the antenna accommodating chamber 80A at a pressure lower than that in the film formation station ST, the reactive gas in the gas bottle 76 is introduced into the film formation station via the mass flow controller 77. ST. A voltage of 13.56 MHz is applied to the antennas 85a, b from the high-frequency power source 89 to cause a high-frequency current to flow. Thereby, plasma is prevented from being generated in the antenna storage chamber 80A, and the antennas 85a and b receive the supply of electric power from the high-frequency power source 89, and an induced electric field is generated inside the film formation station ST to generate plasma of the reactive gas.

在各成膜站ST內,靶材機構61設於成膜站ST之基板搬送方向中央, 自由基源80於靶材機構61之基板搬送方向下游側配置有一個。 In each film formation station ST, the target mechanism 61 is provided at the center of the substrate transfer direction of the film formation station ST. The radical source 80 is disposed on the downstream side of the target mechanism 61 in the substrate transport direction.

構成成膜室21之成膜站ST(ST1~STn)之數目被決定為成膜之多層膜之層數以上之數目。在設置與成膜之多層膜之層數一致之數目之成膜站ST時,各成膜站ST係逐層成膜。在設置較成膜之多層膜之層數多之數目之成膜站ST時,多數層中之至少一層係以複數個成膜站ST成膜。 The number of film formation stations ST (ST1 to STn) constituting the film forming chamber 21 is determined as the number of layers of the multilayer film formed. When the number of the film formation stations ST corresponding to the number of layers of the multilayer film formed is set, each film formation station ST is formed into a film layer by layer. When a film formation station ST having a larger number of layers than the multilayer film is formed, at least one of the plurality of layers is formed by a plurality of film formation stations ST.

裝載用空間部22、卸載用空間部23除了於內部未設置有靶材機構61及自由基源80這點以外,與成膜站ST為相同之構成。 The loading space portion 22 and the unloading space portion 23 have the same configuration as the film forming station ST except that the target mechanism 61 and the radical source 80 are not provided inside.

本實施形態中,雖係在各成膜站ST內,自由基源80於靶材機構61下游側僅配置有一個,但亦可如圖5之濺鍍裝置1′,係在各成膜站ST內,一對自由基源80以夾靶材機構61之方式配置於靶材機構61之上游側與下游側。濺鍍裝置1′之其他構成由於與濺鍍裝置1相同,因此省略說明。 In the present embodiment, although only one of the radical source 80 is disposed on the downstream side of the target mechanism 61 in each of the film formation stations ST, the sputtering apparatus 1' of FIG. 5 may be attached to each film formation station. In the ST, the pair of radical sources 80 are disposed on the upstream side and the downstream side of the target mechanism 61 so as to sandwich the target mechanism 61. Since the other structure of the sputtering apparatus 1' is the same as that of the sputtering apparatus 1, description is abbreviate|omitted.

此外,自由基源亦可於靶材機構61上游側僅配置有一個。 Further, the radical source may be disposed only on the upstream side of the target mechanism 61.

(薄膜形成方法) (film formation method)

以下,說明使用本實施形態之濺鍍裝置1之薄膜形成方法。 Hereinafter, a film forming method using the sputtering apparatus 1 of the present embodiment will be described.

首先,將成膜室21內真空排氣。其次,準備既定數目之於未圖示之基板保持具保持有大尺寸基板43者。開放閘閥12,對濺鍍裝置1之裝載鎖固室11導入既定數目之基板43,關閉閘閥12。將裝載鎖固室11從大氣狀態真空排氣至成為與成膜室21之真空度同等為止。 First, the inside of the film forming chamber 21 is evacuated. Next, a predetermined number of substrate holders (not shown) are prepared to hold the large-sized substrate 43. The gate valve 12 is opened, and a predetermined number of substrates 43 are introduced into the load lock chamber 11 of the sputtering apparatus 1, and the gate valve 12 is closed. The load lock chamber 11 is evacuated from the atmospheric state until it reaches the same degree of vacuum as the film formation chamber 21.

其後,使各成膜站ST之靶材機構61及自由基源80作動,開始濺鍍,開放閘閥13,將第一基板43導入成膜室21之裝載用空間部22。 Then, the target mechanism 61 and the radical source 80 of each film formation station ST are actuated to start sputtering, and the gate valve 13 is opened, and the first substrate 43 is introduced into the mounting space portion 22 of the film forming chamber 21.

藉由未圖示之基板搬送機構,使基板43以一定速度往成膜站STn之方向移動,依序在成膜站ST1至STn進行成膜。 By the substrate transfer mechanism (not shown), the substrate 43 is moved in the direction of the film formation station STn at a constant speed, and film formation is performed in the film formation stations ST1 to STn in this order.

在成膜站ST1至STn之各個,如下述般進行金屬化合物之成膜。 Film formation of a metal compound is performed in each of the film formation stations ST1 to STn as follows.

藉由基板搬送機構搬送之基板43被導入最初之成膜站ST1後,基板43從基板搬送方向上游側依序被導入圖2所示之成膜有效區域A。 After the substrate 43 conveyed by the substrate transfer mechanism is introduced into the first film formation station ST1, the substrate 43 is sequentially introduced into the film formation effective region A shown in FIG. 2 from the upstream side in the substrate transfer direction.

在基板43進入成膜有效區域A後,首先,在濺鍍步驟從靶材63a,b藉由濺鍍擊出金屬粒子,在成膜有效區域A與靶材63a,b所包圍之區域,從靶材63a,b往基板43飛散。 After the substrate 43 enters the film formation effective region A, first, in the sputtering step, the metal particles are struck from the targets 63a, b by sputtering, and the regions surrounded by the film formation effective region A and the targets 63a, b are The targets 63a, b scatter toward the substrate 43.

其次,在飛散中之金屬粒子之一部分於從靶材63a,b至到達基板43之期間,藉由以自由基源80形成之反應性氣體之自由基而成為金屬不完全反應物。此金屬粒子、金屬不完全反應物,相當於申請專利範圍之非完全化合物之粒子。 Next, one of the metal particles in the scattering portion becomes a metal incomplete reactant by the radical of the reactive gas formed by the radical source 80 during the period from the target 63a, b to the substrate 43. The metal particles and the metal incomplete reactant correspond to particles of the incomplete compound of the patent application.

接著,於基板43上堆積金屬粒子與金屬不完全反應物,形成非完全化合物之薄膜形成物。 Next, metal particles and metal incomplete reactants are deposited on the substrate 43 to form a film formation of the incomplete compound.

接著,在組成轉換步驟,藉由以自由基源80形成之反應性氣體之自由基,基板43上之非完全化合物之薄膜形成物被轉換為金屬之完全化合物。 Next, in the composition conversion step, the film formation of the incomplete compound on the substrate 43 is converted into a complete compound of the metal by the radical of the reactive gas formed by the radical source 80.

在基板43通過成膜有效區域A內之期間,並行反覆濺鍍步驟、組成轉換步驟,當基板43從成膜有效區域A被排出時,於基板43上形成有金屬化合物薄膜。 While the substrate 43 passes through the film formation effective region A, the sputtering step and the composition conversion step are performed in parallel, and when the substrate 43 is discharged from the film formation effective region A, a metal compound film is formed on the substrate 43.

在第二次以後之成膜站ST2~n,亦進行與成膜站ST1相同之步驟,而分別形成由金屬之完全化合物構成之薄膜。 At the film formation stations ST2 to n after the second time, the same steps as those of the film formation station ST1 are performed, and a film made of a complete compound of metal is formed.

靶材63a,b之金屬之組合在相鄰之成膜站STi~STi+m(i及m為正整數)中為相同時,在此相鄰之成膜站STi~STi+m中形成相同層之薄膜。亦即,在相鄰之成膜站STi~STi+m中形成一層薄膜。 When the combination of the metals of the targets 63a and b is the same in the adjacent film formation stations STi to STi+m (i and m are positive integers), the same is formed in the adjacent film formation stations STi to STi+m. Film of the layer. That is, a film is formed in the adjacent film formation stations STi to STi+m.

另一方面,靶材63a,b之金屬之組合在相鄰之成膜站STi~STi+m(i及m為正整數)中為不同時,在此相鄰之成膜站STi~STi+m中形成複數層之薄膜。 On the other hand, when the combination of the metals of the targets 63a, b is different in the adjacent film forming stations STi to STi+m (i and m are positive integers), the adjacent film forming stations STi~STi+ A film of a plurality of layers is formed in m.

在進行靶材63a,b之濺鍍、藉自由基源80之反應性氣體之自由基形成之期間,成膜速率係被未圖示之光學式成膜速率控制機構控制,成膜速率控制機構,根據以未圖示之光纖檢測之金屬、氣體、金屬化合物量之資料 控制質流控制器66、77而控制氣體流量,藉此將成膜速率控制成所欲之值。藉此,控制各成膜站ST中之膜厚。 During the sputtering of the targets 63a, b and the radical formation of the reactive gas by the radical source 80, the film formation rate is controlled by an optical film formation rate control mechanism (not shown), and a film formation rate control mechanism According to the amount of metal, gas, and metal compound detected by an optical fiber (not shown) The mass flow controllers 66, 77 are controlled to control the gas flow rate, thereby controlling the film formation rate to a desired value. Thereby, the film thickness in each film formation station ST is controlled.

在成膜站STn之成膜、反應完成後,基板43被導入卸載用空間部23。卸載室31係預先真空排氣成與成膜室21大致相同之真空度。開放閘閥33並將基板43導入卸載室31後,關閉閘閥33,將基板43保持於卸載室31。 After the film formation station STn is formed and the reaction is completed, the substrate 43 is introduced into the unloading space portion 23. The unloading chamber 31 is evacuated in advance to have substantially the same degree of vacuum as the film forming chamber 21. After the gate valve 33 is opened and the substrate 43 is introduced into the unloading chamber 31, the gate valve 33 is closed, and the substrate 43 is held in the unloading chamber 31.

其次,將保持於裝載鎖固室11之次一基板43導入成膜室21,進行相同之成膜、反應厚,同樣地導入卸載室31並加以保持。針對保持於裝載鎖固室11之所有基板43進行相同之處理完成後,使卸載室31成為大氣狀態,開放閘閥32,將所有基板43取出至大氣中,完成成膜。 Next, the next substrate 43 held in the load lock chamber 11 is introduced into the film forming chamber 21, and the same film formation and thick reaction are carried out, and the same is introduced into the unloading chamber 31 and held therein. After the same processing is completed for all the substrates 43 held in the load lock chamber 11, the unloading chamber 31 is brought to an atmospheric state, the gate valve 32 is opened, and all the substrates 43 are taken out to the atmosphere to complete film formation.

藉由以上之方法,形成與成膜站ST數目與金屬及反應氣體之種類對應之層數之金屬化合物之多層膜。 By the above method, a multilayer film of a metal compound having a number of layers corresponding to the number of metals and reaction gases of the film formation station ST is formed.

在所有相鄰之成膜站ST間使用不同金屬及反應氣體時,多層膜會成為與成膜站ST數目對應之層數。在相鄰之成膜站ST間使用相同金屬及反應氣體時,在該相鄰之成膜站ST會一起成膜出一層。 When different metals and reaction gases are used between all adjacent film formation stations ST, the multilayer film becomes the number of layers corresponding to the number of film formation stations ST. When the same metal and the reaction gas are used between the adjacent film formation stations ST, a layer is formed together at the adjacent film formation station ST.

[實施例] [Examples]

以下說明本發明之具體實施例。 Specific embodiments of the invention are described below.

(實驗例1) (Experimental Example 1)

本實驗例中,係將自由基源80設置成介電體板83之面與基板43平行且與靶材63a,b平行,針對使成膜站ST中之基板43與靶材63a,b間之距離D分別變化成40mm、70mm、200mm、400mm之實施例1~4進行成膜,並就成膜速率及所製得之膜作了對比。 In the present experimental example, the radical source 80 is disposed such that the surface of the dielectric plate 83 is parallel to the substrate 43 and parallel to the targets 63a, b, for the substrate 43 in the film formation station ST and the target 63a, b Films of Examples 1 to 4 in which the distance D was changed to 40 mm, 70 mm, 200 mm, and 400 mm, respectively, were formed, and the film formation rate and the obtained film were compared.

本實施例中,使用具備一個成膜站ST之濺鍍裝置1,藉由上述之實施形態之薄膜形成方法於大小600cm×400cm之大型玻璃基板上形成二氧化矽之單層膜。 In the present embodiment, a single-layer film of cerium oxide is formed on a large-sized glass substrate having a size of 600 cm × 400 cm by the thin film forming method of the above-described embodiment using a sputtering apparatus 1 having one film forming station ST.

在成膜站ST1,靶材63a,b使用矽靶材,從氣體瓶65供應作為濺鍍氣 體之氬氣800sccm。導入作為反應性氣體之氧(O2)氣80sccm,藉由自由基源80作成自由基。 In the film formation station ST1, the target materials 63a, b use a ruthenium target, and argon gas 800 sccm as a sputtering gas is supplied from the gas bottle 65. An oxygen (O 2 ) gas as a reactive gas was introduced at 80 sccm, and a radical was generated by the radical source 80.

將其他具體條件及結果顯示於表1。 Other specific conditions and results are shown in Table 1.

從表1之結果可知,在距離D為40mm之情形,所形成之膜之吸收係數為較高之10-3左右。其原因被認為是若距離D過短,則成膜速率變得過高,反應追隨不上而產生吸收之故。 As is clear from the results of Table 1, in the case where the distance D is 40 mm, the absorption coefficient of the formed film is about 10 - 3 higher. The reason for this is considered to be that if the distance D is too short, the film formation rate becomes too high, and the reaction does not follow and causes absorption.

在光學薄膜之情形,為了得到必要之透射率,由於必需有10-4程度之吸收係數,因此可知距離D必需較40mm長。 In the case of an optical film, in order to obtain the necessary transmittance, since it is necessary to have an absorption coefficient of about 10 -4 , it is understood that the distance D must be longer than 40 mm.

(實驗例2) (Experimental Example 2)

本實驗例中,係將成膜站ST中之基板43與靶材63a,b間之距離D設為200mm,將自由基源80傾斜成介電體板83之面往靶材63a,b側傾斜,針對相對基板43變化成0°、30°、60°之實施例3、5、6進行成膜,並就成膜速率及所製得之膜作了對比。 In the present experimental example, the distance D between the substrate 43 and the targets 63a, b in the film formation station ST was set to 200 mm, and the radical source 80 was inclined to the surface of the dielectric plate 83 toward the target 63a, b side. Incident, the film formation was carried out for Examples 3, 5, and 6 in which the opposite substrate 43 was changed to 0, 30, and 60, and the film formation rate and the obtained film were compared.

將其他具體條件及結果顯示於表2。又,本實驗例之其他條件與實驗例1相同。 Other specific conditions and results are shown in Table 2. Further, other conditions of the experimental example were the same as those of Experimental Example 1.

從表2之結果可知,在介電體板83之面相對基板43傾斜30°、60°之情形,成膜速率較未傾斜之情形變得更高。因此,可知藉由使自由基源80往靶材63a,b傾斜,由於可在保持適度吸收係數之狀態下使反應性提升,因此能提高靶材功率,謀求成膜速率之更加提升。 As is clear from the results of Table 2, in the case where the surface of the dielectric plate 83 is inclined by 30° and 60° with respect to the substrate 43, the film formation rate becomes higher than that without tilting. Therefore, it is understood that by tilting the radical source 80 toward the targets 63a and b, the reactivity can be improved while maintaining a moderate absorption coefficient, so that the target power can be increased and the film formation rate can be further improved.

(實驗例3) (Experimental Example 3)

本實驗例中,係於具備一個成膜站ST之濺鍍裝置1中,針對具備單一自由基源80之情形與於夾靶材63a,b之上游側及下游側具備一對自由基源80之情形進行成膜,並就成膜速率及所製得之膜作了對比。 In the present experimental example, in the sputtering apparatus 1 including one film formation station ST, a pair of radical sources 80 are provided on the upstream side and the downstream side of the clip target 63a, b in the case where the single radical source 80 is provided. In the case of film formation, the film formation rate and the obtained film were compared.

將其他具體條件及結果顯示於表3。又,本實驗例之其他條件與實驗例1相同。 Other specific conditions and results are shown in Table 3. Further, other conditions of the experimental example were the same as those of Experimental Example 1.

從表3之結果可知,具備一對自由基源80之情形、與具備單一自由基源80之情形對比,其吸收係數保持大致相同之值,成膜速率變高一成左右。因此,可知藉由具備一對自由基源80,由於可在保持適度吸收係數之狀態下使反應性提升,因此能提高靶材功率,謀求成膜速率之更加提升。 As is clear from the results of Table 3, in the case where the pair of radical sources 80 are provided, the absorption coefficient is kept substantially the same as that of the case where the single radical source 80 is provided, and the film formation rate is increased by about one percent. Therefore, it is understood that by providing the pair of radical sources 80, the reactivity can be improved while maintaining a moderate absorption coefficient, so that the target power can be increased and the film formation rate can be further improved.

(實驗例4) (Experimental Example 4)

本實驗例中,在使用上述實施形態之濺鍍裝置1形成多層AR膜之情形,進行在單一成膜站ST將各層成膜之實施例8與在複數個成膜站ST成膜之實施例9,並就成膜條件及所製得之膜作了對比。 In the present experimental example, in the case where the multilayer AR film was formed by using the sputtering apparatus 1 of the above-described embodiment, Example 8 in which each layer was formed in a single film formation station ST and an embodiment in which a plurality of film formation stations ST were formed were formed. 9, and the film formation conditions and the prepared film were compared.

實施例8、9之多層AR膜之膜設計,係使第一層為物理膜厚123.9nm之Si3N4、使第二層為物理膜厚164.3nm之SiO2、使第三層為物理膜厚99.5nm 之Si3N4、使第四層為物理膜厚73.2nm之SiO2The film design of the multilayer AR film of Examples 8 and 9 is such that the first layer is Si 3 N 4 having a physical film thickness of 123.9 nm, the second layer is SiO 2 having a physical film thickness of 164.3 nm, and the third layer is made of physics. Si 3 N 4 having a film thickness of 99.5 nm and SiO 2 having a physical thickness of 73.2 nm were used for the fourth layer.

在實施例8中,使用具備四個成膜站ST之濺鍍裝置1,在各成膜站ST1~4中,靶材63a,b使用矽靶材,從氣體瓶65供應作為濺鍍氣體之氬氣800sccm。又,作為反應性氣體,在成膜站ST1、ST3導入氮(N2)氣140sccm、在成膜站ST2、ST4導入氧(O2)氣60sccm,藉由自由基源80作成自由基。在各成膜站ST1~4分別成膜出Si3N4、SiO2、Si3N4、SiO2In the eighth embodiment, a sputtering apparatus 1 having four film formation stations ST is used. In each of the film formation stations ST1 to 4, the target materials 63a, b are supplied with a target material, and the gas bottle 65 is supplied as a sputtering gas. Argon gas was 800 sccm. Further, as a reactive gas, nitrogen (N 2 ) gas was introduced into the film formation stations ST1 and ST3 at 140 sccm, and oxygen (O 2 ) gas was introduced into the film formation stations ST2 and ST4 at 60 sccm, and radicals were formed by the radical source 80. Si 3 N 4 , SiO 2 , Si 3 N 4 , and SiO 2 are formed in each of the film formation stations ST1 to S4.

又,基板搬送速度為4.4mm/s,距離D為200mm,介電體板83與基板43之角度為30°。 Further, the substrate transport speed was 4.4 mm/s, the distance D was 200 mm, and the angle between the dielectric plate 83 and the substrate 43 was 30°.

將實施例8之其他具體條件及結果顯示於表4。 Further specific conditions and results of Example 8 are shown in Table 4.

在實施例9中,使用具備七個成膜站ST之濺鍍裝置1,在各成膜站ST1~7中,在每一相鄰之一對成膜站ST形成相同組成之膜,而形成合計三層之Si3N4、SiO2、Si3N4。在成膜站ST7,係以單一之成膜站ST形成最上層之SiO2膜。所形成之四層之膜厚分別與實施例8之四層之膜厚相同。 In the ninth embodiment, a sputtering apparatus 1 having seven film forming stations ST is used, and in each of the film forming stations ST1 to 7, a film of the same composition is formed at each adjacent one of the film forming stations ST to form a film. A total of three layers of Si 3 N 4 , SiO 2 , and Si 3 N 4 are used . In the film formation station ST7, the uppermost layer of SiO 2 film is formed by a single film formation station ST. The film thicknesses of the four layers formed were the same as those of the four layers of Example 8.

又,基板搬送速度為8.7mm/s,距離D為200mm,介電體板83與基板43之角度為30°。 Further, the substrate transport speed was 8.7 mm/s, the distance D was 200 mm, and the angle between the dielectric plate 83 and the substrate 43 was 30°.

將實施例9之其他具體條件及結果顯示於表5。 Further specific conditions and results of Example 9 are shown in Table 5.

根據實驗例4,即使係在每一層具備複數個成膜站ST之實施例9,亦形成有與在每一層具備單數成膜站ST之實施例8大致相同膜厚之膜。又,實施例9中,基板搬送速度雖為實施例8之情形之大致一倍,但由於至第三層為止係在兩個成膜站ST成膜,因此一片基板43之成膜所花費之時間在實施例9與實施例8為相同。 According to Experimental Example 4, even in Example 9 in which a plurality of film formation stations ST were provided in each layer, a film having a film thickness substantially the same as that of Example 8 having a single film formation station ST in each layer was formed. Further, in the ninth embodiment, the substrate transport speed is substantially doubled as in the case of the eighth embodiment. However, since the film formation is performed at the two film formation stations ST until the third layer, the film formation of one substrate 43 is required. The time is the same in the embodiment 9 and the eighth embodiment.

然而,實施例9,由於基板搬送速度較實施例8快,濺鍍裝置1所含之成膜站ST之數目較多,因此在以直列式連續地使基板43移動於濺鍍裝置1內時,能同時存在於濺鍍裝置1內之基板43數目變多,生產性提升。 However, in the ninth embodiment, since the substrate transport speed is faster than that of the eighth embodiment, the number of the film formation stations ST included in the sputtering apparatus 1 is large, and therefore, when the substrate 43 is continuously moved in the sputtering apparatus 1 in an in-line manner The number of the substrates 43 which can be simultaneously present in the sputtering apparatus 1 is increased, and the productivity is improved.

圖6係顯示以實施例9成膜之多層AR膜在各波長之反射率、以及使第一層為物理膜厚123.9nm之Si3N4、使第二層為物理膜厚164.3nm之SiO2、使第三層為物理膜厚99.5nm之Si3N4、使第四層為物理膜厚73.2nm之SiO2之多層AR膜之膜設計在各波長之反射率對比後之圖表。 6 is a graph showing the reflectance of the multilayer AR film formed in Example 9 at each wavelength, and the Si 3 N 4 having a first layer of a physical film thickness of 123.9 nm and the second layer being a physical film thickness of 164.3 nm. 2. A graph in which the third layer is a Si 5 N 4 film having a physical film thickness of 99.5 nm, and a film of a multilayer AR film having a fourth layer of SiO 2 having a physical film thickness of 73.2 nm is designed to reflect the reflectance at each wavelength.

如圖6所示,可知以實施例9形成之多層AR膜,可取得接近膜設計之光學特性。 As shown in Fig. 6, it is understood that the multilayer AR film formed in Example 9 can achieve optical characteristics close to the film design.

(實驗例5) (Experimental Example 5)

本實驗例中,氧氣流量以外之條件與實驗例3之條件相同,在使氧氣流量從0sccm增加至200sccm之情形與從200sccm減少至0sccm之情形,測定在0、60、70、80、90、110、120、130、150、200sccm之靶材電壓,確認 在氧氣流量增加之情形與減少之情形中,是否產生相對於氧分壓之靶材電壓之變化路徑相異之所謂滯後現象。 In the experimental example, the conditions other than the oxygen flow rate were the same as those of the experimental example 3, and the case where the oxygen flow rate was increased from 0 sccm to 200 sccm and the case where the oxygen flow rate was decreased from 200 sccm to 0 sccm was measured at 0, 60, 70, 80, 90, 110, 120, 130, 150, 200 sccm target voltage, confirmation In the case where the oxygen flow rate is increased and decreased, whether or not a so-called hysteresis is generated which is different from the change path of the target voltage of the oxygen partial pressure.

將氧氣流量、氧氣分壓、增加時及減少時之靶材電壓之資料顯示於表6,將顯示氧分壓與增加時及減少時之靶材電壓之關連之圖表顯示於圖7。 The data of the oxygen flow rate, oxygen partial pressure, increase and decrease target voltage are shown in Table 6. The graph showing the relationship between the oxygen partial pressure and the target voltage at the time of increase and decrease is shown in Fig. 7.

從圖7可知,在氧氣流量增加之情形與氧氣流量減少之情形,相對於氧分壓之靶材電壓之變化路徑為大致相同,未產生會在反應性濺鍍中產生之滯後現象。 As can be seen from Fig. 7, in the case where the oxygen flow rate is increased and the oxygen flow rate is decreased, the change path of the target voltage with respect to the oxygen partial pressure is substantially the same, and no hysteresis which occurs in the reactive sputtering is generated.

因此,使用本例之濺鍍裝置1,藉由上述之實施形態之薄膜形成方法濺鍍時,可知與反應性濺鍍不同地,藉由調整氧氣流量而進行之成膜速率之控制係容易。 Therefore, when the sputtering apparatus 1 of the present embodiment is used for sputtering by the thin film formation method of the above-described embodiment, it is understood that the control of the deposition rate by adjusting the oxygen flow rate is different from that of the reactive sputtering.

A‧‧‧成膜有效區域 A‧‧‧ filming effective area

D‧‧‧距離 D‧‧‧Distance

ST‧‧‧成膜站 ST‧‧‧ filming station

43‧‧‧基板 43‧‧‧Substrate

61‧‧‧靶材機構 61‧‧‧ Target Agency

62a,62b‧‧‧磁控濺鍍電極 62a, 62b‧‧‧Magnetron Sputtering Electrodes

63a,63b‧‧‧靶材 63a, 63b‧‧‧ targets

64‧‧‧交流電源 64‧‧‧AC power supply

65,76‧‧‧氣體瓶 65,76‧‧‧ gas bottles

66,77‧‧‧質流控制器 66,77‧‧‧Flow Controller

75,95a‧‧‧配管 75, 95a‧‧‧Pipe

80‧‧‧自由基源 80‧‧‧Free radical source

83‧‧‧介電體板 83‧‧‧Dielectric board

87‧‧‧匹配箱 87‧‧‧match box

89‧‧‧高頻電源 89‧‧‧High frequency power supply

95‧‧‧真空泵 95‧‧‧vacuum pump

Claims (15)

一種薄膜形成裝置,係在真空槽內,藉由濺鍍於基板上形成金屬化合物之薄膜,其特徵在於:於前述真空槽內具備:靶材,由金屬或具有導電性之金屬化合物構成;以及活性種源,設成與該靶材相互在電磁性及壓力上彼此影響,生成反應性氣體之活性種;前述靶材,與前述基板對向配置;前述活性種源,具備供應前述反應性氣體之氣體源、以及將能量供應至前述真空槽內以將前述反應性氣體激發成電漿狀態之能量源;前述能量源,在與前述真空槽之間具備用以將前述能量供應至前述真空槽內之介電體窗;該介電體窗,配置成相對位於與前述能量源對向之位置之前述基板以90°未滿之角度往前述靶材側傾斜。 A thin film forming apparatus which is formed by sputtering a thin film of a metal compound on a substrate in a vacuum chamber, wherein the vacuum chamber is provided with a target material composed of a metal or a conductive metal compound; The active seed source is formed to interact with the target electromagnetically and under pressure to generate an active species of a reactive gas; the target material is disposed opposite to the substrate; and the active seed source is provided with the reactive gas a gas source and an energy source for supplying energy into the vacuum chamber to excite the reactive gas into a plasma state; the energy source being provided between the vacuum chamber and the vacuum chamber for supplying the energy to the vacuum chamber a dielectric window; the dielectric window is disposed to be inclined toward the target side at an angle of less than 90° with respect to the substrate located at a position opposite to the energy source. 如申請專利範圍第1項之薄膜形成裝置,其中,前述介電體窗,配置成相對前述基板以30°以上之角度往前述靶材側傾斜,前述基板係在相對前述基板之搬送方向為垂直之方向位於與前述能量源對向之位置。 The thin film forming apparatus according to claim 1, wherein the dielectric window is disposed to be inclined toward the target side at an angle of 30 or more with respect to the substrate, and the substrate is perpendicular to a transport direction of the substrate. The direction is located opposite the aforementioned energy source. 如申請專利範圍第1項之薄膜形成裝置,其具備在前述真空槽內搬送前述基板之基板搬送單元;於前述靶材之前述基板之搬送方向之上游側及下游側中之至少一方具備前述活性種源。 The film forming apparatus according to the first aspect of the invention, comprising: a substrate transport unit that transports the substrate in the vacuum chamber; and at least one of an upstream side and a downstream side of a transport direction of the substrate in the target material; Source. 如申請專利範圍第1項之薄膜形成裝置,其具備在前述真空槽內搬送前述基板之基板搬送單元;於前述靶材之前述基板之搬送方向之上游側及下游側具備前述活性種源。 The film forming apparatus according to the first aspect of the invention, comprising: a substrate transfer unit that transports the substrate in the vacuum chamber; and the active seed source on an upstream side and a downstream side of a transport direction of the substrate in the target material. 如申請專利範圍第1項之薄膜形成裝置,其中,控制往前述靶材導入之濺鍍氣體之流量之濺鍍氣體控制器與控制前述反應性氣體之流量之反應性氣體控制器係相互獨立設置;且具備以光學方式檢測成膜速率之檢測部;並具備控制裝置,該控制裝置係接收來自該檢測部之訊號,至少獨立控制前述濺鍍之電源及前述濺鍍氣體控制器、以及前述活性種源之電源及前述反應性氣體控制器,來控制前述成膜速率。 The film forming apparatus of claim 1, wherein the sputtering gas controller for controlling the flow rate of the sputtering gas introduced into the target and the reactive gas controller for controlling the flow rate of the reactive gas are independently set And a detection unit for optically detecting a film formation rate; and a control device for receiving a signal from the detection unit, at least independently controlling the sputtering power source and the sputtering gas controller, and the activity The source power source and the aforementioned reactive gas controller are used to control the film formation rate. 如申請專利範圍第1或2項之薄膜形成裝置,其中,前述能量源係通過前述介電體窗藉由感應耦合或表面波生成電漿之電漿源。 The film forming apparatus according to claim 1 or 2, wherein the energy source generates a plasma source of plasma by inductive coupling or surface wave through the dielectric window. 如申請專利範圍第1或3項之薄膜形成裝置,其中,前述活性種源係感應耦合型電漿(ICP)自由基源。 The film forming apparatus according to claim 1 or 3, wherein the active seed source is an inductively coupled plasma (ICP) radical source. 如申請專利範圍第3項之薄膜形成裝置,其中,前述薄膜形成裝置係由具備複數個成膜站之直列型濺鍍裝置構成,該成膜站包含前述靶材與設於該靶材之前述基板之搬送方向之上游側及下游側中之至少一方之前述活性種源。 The film forming apparatus according to claim 3, wherein the film forming apparatus comprises an in-line sputtering apparatus including a plurality of film forming stations, wherein the film forming station includes the target and the aforementioned The active seed source of at least one of the upstream side and the downstream side of the substrate transport direction. 如申請專利範圍第8項之薄膜形成裝置,其中,前述成膜站具備以光學方式檢測成膜速率之檢測部;並具備接收來自前述成膜速率之檢測部之訊號,以控制各該前述成膜站之個別成膜速率之控制裝置。 The film forming apparatus according to claim 8, wherein the film forming station includes a detecting unit that optically detects a film forming rate, and includes a signal for receiving a detecting unit from the film forming rate to control each of the forming units. Control device for individual film formation rates of membrane stations. 如申請專利範圍第1或3項之薄膜形成裝置,其具備:濺鍍單元,在前述真空槽內濺鍍前述靶材,藉由該濺鍍從前述靶材使非完全化合物之粒子往基板飛散;以及組成轉換單元,藉由在前述真空槽內,使藉由前述活性種源生成之反應性氣體之活性種接觸於前述粒子,以轉換為金屬之完全化合物;能於前述基板上形成由前述金屬之完全化合物構成之薄膜。 The film forming apparatus according to claim 1 or 3, further comprising: a sputtering unit that sputters the target in the vacuum chamber, and the particles of the incomplete compound are scattered from the target to the substrate by the sputtering And a composition conversion unit, wherein the active species of the reactive gas generated by the active species source are contacted with the particles in the vacuum chamber to be converted into a complete compound of the metal; and the substrate can be formed on the substrate A film composed of a complete compound of metal. 一種濺鍍陰極,係在薄膜形成裝置所具備之真空槽內藉由濺鍍於基板上形成金屬化合物之薄膜,其特徵在於,具備:靶材,由金屬或具有導電性之金屬化合物構成;以及活性種源,設成與該靶材相互在電磁性及壓力上彼此影響,生成反應性氣體之活性種;前述活性種源,具備供應前述反應性氣體之氣體源、以及將能量供應至前述真空槽內以將前述反應性氣體激發成電漿狀態之能量源;前述靶材,與前述基板對向配置;前述能量源,具備用以將前述能量供應至前述能量源外部之介電體窗;該介電體窗,配置成相對位於與前述能量源對向之位置之前述基板以90°未滿之角度往前述靶材側傾斜。 A sputtering cathode is a film in which a metal compound is formed by sputtering on a substrate in a vacuum chamber provided in a thin film forming apparatus, and comprises: a target material made of a metal or a conductive metal compound; The active seed source is formed to interact with the target electromagnetically and under pressure to generate an active species of the reactive gas; the active seed source has a gas source for supplying the reactive gas, and supplies energy to the vacuum An energy source for exciting the reactive gas into a plasma state in the tank; the target material is disposed opposite to the substrate; and the energy source is provided with a dielectric window for supplying the energy to the outside of the energy source; The dielectric window is disposed to be inclined toward the target side at an angle of less than 90° with respect to the substrate located at a position opposite to the energy source. 如申請專利範圍第11項之濺鍍陰極,其中,前述靶材與前述活性種源於真空槽之同一空間內並置成產生濺蝕之前述靶材之濺鍍面與前述活性種源對向於前述基板、前述活性種源位於前述靶材之前述基板之搬送方向之上游側及下游側中之至少一方。 The sputter cathode of claim 11, wherein the target material and the active species are sourced in the same space of the vacuum chamber, and the sputtered surface of the target which is sputtered is opposed to the active seed source. The substrate and the active species source are located at least one of an upstream side and a downstream side in a transport direction of the substrate of the target. 一種薄膜形成方法,其具備:濺鍍步驟,在真空槽內,濺鍍與基板對向配置之由金屬或具有導電性之金屬化合物構成之靶材,藉由該濺鍍從前述靶材使非完全化合物之粒子往前述基板飛散;以及組成轉換步驟,具備用以在前述真空槽內,相對位於與前述能量源對向之位置之前述基板以90°未滿之角度往前述靶材側傾斜以將能量供應至前述真空槽內的介電體窗,使藉由設成與前述靶材相互在電磁性及壓力上彼此影響之生成反應性氣體之活性種之活性種源生成之反應性氣體之活性種接觸於前述粒子,以轉換為金屬之完全化合物;藉由具備上述兩步驟,於前述基板上形成由前述金屬之完全化合物構 成之薄膜。 A method for forming a thin film, comprising: a sputtering step of sputtering a target made of a metal or a conductive metal compound disposed opposite to a substrate in a vacuum chamber, wherein the sputtering is performed from the target a particle of the complete compound is scattered toward the substrate; and a composition conversion step is provided, wherein the substrate in the vacuum chamber is inclined toward the target side at an angle of less than 90° with respect to the substrate located opposite to the energy source Supplying energy to the dielectric window in the vacuum chamber to generate a reactive gas generated by an active species source of an active species that forms a reactive gas that is electromagnetically and pressure-sensitive to each other The active species is contacted with the particles to be converted into a complete compound of the metal; by having the above two steps, a complete compound of the foregoing metal is formed on the substrate Into the film. 如申請專利範圍第13項之薄膜形成方法,其中,在前述組成轉換步驟後進行反覆成膜步驟,該反覆成膜步驟係將前述濺鍍步驟及前述組成轉換步驟並行反覆複數次。 The film forming method of claim 13, wherein the reverse film forming step is performed by repeating the sputtering step and the composition converting step in parallel after the composition converting step. 如申請專利範圍第13或14項之薄膜形成方法,其中,在前述濺鍍步驟前進行對具備複數個成膜站之直列型薄膜形成裝置導入前述基板之步驟,該成膜站包含前述靶材與設於該靶材之前述基板之搬送方向之上游側及下游側中之至少一方之前述活性種源;進行站內成膜步驟,該站內成膜步驟係在前述成膜站內將前述基板一邊以一定速度搬送、一邊進行前述濺鍍步驟、前述組成轉換步驟、前述反覆成膜步驟;進行將前述基板搬送至前述基板之搬送方向之前述下游側之前述成膜站之搬送步驟;進行反覆前述站內成膜步驟與前述搬送步驟之複數站成膜步驟;在位於前述基板之搬送方向之最下游之前述成膜站進行前述站內成膜步驟後,進行將前述基板排出至大氣中之步驟。 The method for forming a film according to claim 13 or 14, wherein the step of introducing the substrate into an in-line type thin film forming apparatus including a plurality of film forming stations, wherein the film forming station includes the target material, is performed before the sputtering step And an active seed source provided on at least one of an upstream side and a downstream side of a transport direction of the substrate of the target; and an in-station film forming step of forming the substrate in the film forming station Carrying out the sputtering step, the composition conversion step, and the reverse film formation step at a constant speed, and performing a transfer step of transporting the substrate to the film formation station on the downstream side in the transport direction of the substrate; and repeating the above-mentioned station The film forming step and the plurality of station forming steps of the transporting step; and the step of discharging the substrate into the atmosphere after performing the in-situ film forming step at the film forming station located at the most downstream of the substrate transport direction.
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